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  1. .gitattributes +73 -0
  2. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/README.md +16 -0
  3. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/figures/survivors.tex +27 -0
  4. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/main.tex +109 -0
  5. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/references.bib +217 -0
  6. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/certificates.tex +631 -0
  7. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/derandomization.tex +585 -0
  8. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/inequality.tex +365 -0
  9. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/introduction.tex +196 -0
  10. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/preliminaries.tex +104 -0
  11. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/preparation.tex +526 -0
  12. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/rounding.tex +871 -0
  13. preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/main.pdf +3 -0
  14. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/README.md +18 -0
  15. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/bibliography.tex +130 -0
  16. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/figures/endpoint-slices.tex +22 -0
  17. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/main.tex +64 -0
  18. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/01-forms.tex +48 -0
  19. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/01-introduction.tex +227 -0
  20. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/02-filtered.tex +231 -0
  21. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/03-monomial.tex +218 -0
  22. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/04-stabilization.tex +216 -0
  23. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/05-boxes.tex +269 -0
  24. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/06-tor.tex +256 -0
  25. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/07-assembly.tex +53 -0
  26. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/08-characteristic-zero.tex +85 -0
  27. preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/paper.pdf +3 -0
  28. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/README.md +18 -0
  29. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026.pdf +3 -0
  30. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/main.tex +63 -0
  31. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/references.bib +267 -0
  32. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/01-introduction.tex +286 -0
  33. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/02-framework.tex +75 -0
  34. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/03-metric.tex +262 -0
  35. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/04-filtrations.tex +276 -0
  36. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/05-surgery.tex +249 -0
  37. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/06-chains.tex +324 -0
  38. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/07-idempotents.tex +258 -0
  39. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/08-detector.tex +203 -0
  40. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/09-completion.tex +144 -0
  41. preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/10-torsion-free.tex +121 -0
  42. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/README.md +18 -0
  43. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/figures/field-tower.tex +40 -0
  44. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/figures/proof-interfaces.tex +54 -0
  45. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/paper.tex +103 -0
  46. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/references.bib +448 -0
  47. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/consequences.tex +171 -0
  48. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/differentials.tex +782 -0
  49. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/foundations.tex +167 -0
  50. preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/group.tex +839 -0
.gitattributes CHANGED
@@ -621,3 +621,76 @@ preprints/Termination-for-projective-log-canonical-fourfolds-with-rational-bound
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  preprints/Termination-of-generalized-canonical-flips-on-compact-Kahler-fourfolds-October-5-2026/termination-generalized-terminal-flips-compact-kahler-fourfolds.pdf filter=lfs diff=lfs merge=lfs -text
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  preprints/Termination-of-generalized-log-canonical-flips-on-compact-Kahler-fourfolds-October-5-2026/termination-generalized-lc-kahler-fourfolds.pdf filter=lfs diff=lfs merge=lfs -text
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  preprints/The-Abelian-Zilber-Pink-Conjecture-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
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  preprints/Termination-of-generalized-canonical-flips-on-compact-Kahler-fourfolds-October-5-2026/termination-generalized-terminal-flips-compact-kahler-fourfolds.pdf filter=lfs diff=lfs merge=lfs -text
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  preprints/Termination-of-generalized-log-canonical-flips-on-compact-Kahler-fourfolds-October-5-2026/termination-generalized-lc-kahler-fourfolds.pdf filter=lfs diff=lfs merge=lfs -text
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  preprints/The-Abelian-Zilber-Pink-Conjecture-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-abelianity-conjecture-for-special-compact-Kahler-manifolds-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/the-additive-indecomposability-of-the-primes-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-affine-Bernstein-theorem-in-dimensions-three-through-nine-September-24-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-arithmetic-category-and-stable-recovery-of-lattice-factors-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Bogomolov-Pop-reconstruction-theorem-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Boltzmann-Grad-limit-for-stable-radial-potentials-on-regular-kinetic-intervals-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Campana-Peternell-conjecture-in-dimension-six-September-25-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-canonical-massive-continuum-limit-of-the-two-dimensional-O3-model-October-4-2026/massive-continuum-o3.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-circulant-Hadamard-conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-complete-Crouzeix-theorem-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-complexity-of-identifying-a-graph-by-Weisfeiler-Leman-refinement-September-25-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-cotype-cotype-conjecture-under-the-approximation-property-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-critical-correlation-exponent-of-the-planar-XY-model-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-critical-dimension-for-one-phase-Bernoulli-minimizers-September-24-2026/The-critical-dimension-for-one-phase-Bernoulli-minimizers-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-critical-Liouville-quantum-sphere-and-geometric-limits-of-FK-maps-at-q-equals-4-September-24-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-critical-logarithmic-correction-for-the-planar-XY-model-October-5-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Critical-Spin-Field-of-the-Planar-XY-Model-October-5-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-crossing-number-of-complete-bipartite-graphs-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-crossing-number-of-complete-graphs-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-curve-scaling-limit-of-half-plane-double-dimers-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Deligne-Drinfeld-conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Dimension-of-the-Two-Adic-Hecke-Algebra-at-Odd-Level-October-5-2026/two-adic-hecke.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-dyadic-case-of-the-Erdos-similarity-conjecture-September-25-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-E-times-CM-Component-of-Zilber-Pink-for-Curves-in-A2-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-entropy-photon-number-inequality-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-entropy-rate-dimension-formula-for-self-similar-measures-on-the-line-September-24-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-equivariant-cohomological-Hikita-conjecture-for-arbitrary-quivers-September-24-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Euclidean-plane-is-not-five-colorable-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Euclidean-Steinitz-Bergstrom-theorem-September-24-2026/The-Euclidean-Steinitz-Bergstrom-theorem-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-exact-reconstruction-threshold-for-the-three-state-symmetric-channel-September-25-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Factor-Two-Hardness-Threshold-for-Vertex-Cover-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Falconer-distance-conjecture-in-all-dimensions-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-first-lattice-correction-to-Blochs-law-October-5-2026/first-lattice-correction-bloch-law.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-free-energy-of-the-Ising-random-perceptron-September-24-2026/The-free-energy-of-the-Ising-random-perceptron-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-free-energy-of-the-spherical-random-perceptron-September-24-2026/The-free-energy-of-the-spherical-random-perceptron-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-free-uniform-spanning-forest-is-a-factor-of-IID-September-25-2026/The-free-uniform-spanning-forest-is-a-factor-of-IID-September-25-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Gaussian-free-field-limit-of-integer-Lipschitz-heights-with-two-arc-boundary-data-September-25-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Gaussian-free-field-limit-of-the-balanced-six-vertex-model-with-variance-multiplier-1-over-arcsin-c-over-2-September-23-2026/The-Gaussian-free-field-limit-of-the-balanced-six-vertex-model-with-variance-multiplier-1-over-arcsin-c-over-2-September-23-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Gaussian-Propeller-Bound-in-Every-Dimension-September-24-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Generalized-Mukai-Conjecture-September-24-2026/article.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-geometric-case-of-the-Erdos-similarity-conjecture-October-5-2026/geometric-erdos-similarity.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Grothendieck-homotopy-hypothesis-via-elementary-expansions-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-height-three-chromatic-overlap-an-explicit-filtration-and-its-attachments-September-27-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-higher-dimensional-Erdos-distinct-distances-conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Hilbert-Smith-conjecture-in-every-finite-dimension-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-hypercube-Ramsey-number-has-linear-order-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-irrationality-exponent-of-pi-is-2-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Isoperimetric-Conjecture-for-the-Cubic-Flat-Three-Torus-September-24-2026/article.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-joint-Dickman-law-for-consecutive-integers-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-joint-scaling-limit-of-critical-Ashkin-Teller-currents-September-25-2026/main.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Kakeya-maximal-conjecture-in-three-dimensions-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Kerr-Newman-Penrose-Inequality-for-Axisymmetric-Electrovacuum-Exteriors-October-5-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Kervaire-Invariant-Problem-at-the-Prime-Three-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Kervaire-Theorem-for-Groups-September-24-2026/The-Kervaire-Theorem-for-Groups-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Kirchberg-Rordam-character-criterion-September-25-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-l1-Bass-Conjecture-for-Discrete-Groups-October-5-2026/l1-bass-conjecture.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-logarithmic-Brunn-Minkowski-conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-low-temperature-Sherrington-Kirkpatrick-fluctuation-scale-September-24-2026/The-low-temperature-Sherrington-Kirkpatrick-fluctuation-scale-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-low-temperature-Sherrington-Kirkpatrick-free-energy-limiting-law-September-24-2026/The-low-temperature-Sherrington-Kirkpatrick-free-energy-limiting-law-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
687
+ preprints/The-Mahler-Conjecture-for-General-Convex-Bodies-September-22-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Margulis-Platonov-conjecture-over-global-function-fields-October-5-2026/margulis-platonov-global-function-fields.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Margulis-Platonov-conjecture-over-number-fields-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-maximal-triangular-Hilbert-transform-at-the-symmetric-point-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-maximum-number-of-mutually-unbiased-bases-in-dimension-six-September-24-2026/The-maximum-number-of-mutually-unbiased-bases-in-dimension-six-September-24-2026.pdf filter=lfs diff=lfs merge=lfs -text
692
+ preprints/The-mean-analytic-rank-of-quadratic-twists-of-elliptic-curves-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
693
+ preprints/The-metric-Blaschke-theorem-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-Mezard-Parisi-formula-for-diluted-spin-glasses-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-nonmaximal-anti-de-Sitter-Penrose-Inequality-and-original-data-rigidity-October-5-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/The-normalized-volume-gap-in-dimension-four-September-24-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/README.md ADDED
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+ # [The approximation threshold for metric k-median](main.pdf)
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+
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+ OpenAI
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+ September 24, 2026
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+
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+ ## Citation
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+
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+ ```bibtex
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+ @misc{OAI:The-Approximation-Threshold-for-Metric-k-Median-September-24-2026,
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+ author = {{OpenAI}},
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+ title = {{The approximation threshold for metric $k$-median}},
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+ howpublished = {OpenAI Math Release preprint
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+ \href{https://github.com/openai/math/blob/main/preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/main.pdf}{OAI:The-Approximation-Threshold-for-Metric-k-Median-September-24-2026}},
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+ year = {2026}
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+ }
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+ ```
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/figures/survivors.tex ADDED
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+ \begin{figure}[tbp]
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+ \centering
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+ \begin{tikzpicture}[
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+ box/.style={draw,rounded corners=2pt,align=center,inner sep=7pt,
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+ text width=3.95cm,font=\small},
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+ flow/.style={-{Stealth[length=2mm]},thick},
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+ note/.style={align=center,font=\small}]
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+ \node[note] (source) {A full update at an alive source $h\in S$ opens its facility};
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+ \node[box,below=10mm of source,xshift=-4.8cm] (erased)
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+ {$S\cap E_h$\\[3pt]Physically erased\\and removed from $S$};
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+ \node[box,right=4mm of erased] (kept)
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+ {$i\in S\setminus E_h$\\with $ad_i<d_h$\\[3pt]Physically survives\\and remains alive};
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+ \node[box,right=4mm of kept] (discarded)
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+ {$i\in S\setminus E_h$\\with $ad_i\ge d_h$\\[3pt]Physically survives;\\discarded from the analysis};
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+ \draw[flow] (source.south) -- ++(0,-4mm) -| (erased.north);
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+ \draw[flow] (source.south) -- (kept.north);
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+ \draw[flow,dashed] (source.south) -- ++(0,-4mm) -| (discarded.north);
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+ \node[box,text width=12.95cm,below=8mm of kept] (reset)
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+ {The opened facility is reset to $\Delta$ active copies.\\
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+ These regenerated copies are not original identities in $S_0$ and do not enter $S$.};
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+ \end{tikzpicture}
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+ \caption{One full source update, with no simultaneous relevant action.
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+ Only the middle group contributes to the continued alive assignment.
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+ The dashed branch is an analysis discard, not a physical erasure.
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+ Positions are schematic and represent no metric geometry.}
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+ \label{fig:survivors}
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+ \end{figure}
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/main.tex ADDED
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46
+ \usepackage{amsmath,amssymb,amsthm,mathtools}
47
+ \usepackage{microtype}
48
+ \usepackage{booktabs,longtable,array}
49
+ \usepackage{enumitem}
50
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51
+ \usepackage{xcolor}
52
+ \usepackage{tikz}
53
+ \usetikzlibrary{arrows.meta,positioning,calc}
54
+ \usepackage[numbers,sort&compress]{natbib}
55
+ \usepackage[colorlinks=true,linkcolor=blue!50!black,citecolor=blue!50!black,urlcolor=blue!50!black]{hyperref}
56
+ \usepackage[figure]{hypcap}
57
+ \usepackage{bookmark}
58
+ \hypersetup{pdftitle={The approximation threshold for metric k-median},pdfauthor={OpenAI}}
59
+ \renewcommand{\bibsection}{\section*{\refname}\addcontentsline{toc}{section}{\refname}}
60
+ \newtheorem{theorem}{Theorem}[section]
61
+ \newtheorem{lemma}[theorem]{Lemma}
62
+ \newtheorem{proposition}[theorem]{Proposition}
63
+ \newtheorem{corollary}[theorem]{Corollary}
64
+ \theoremstyle{definition}
65
+ \newtheorem{definition}[theorem]{Definition}
66
+ \theoremstyle{remark}
67
+ \newtheorem{remark}[theorem]{Remark}
68
+ \newcommand{\E}{\mathbb E}
69
+ \newcommand{\Prob}{\mathbb P}
70
+ \DeclareMathOperator{\Var}{Var}
71
+ \DeclareMathOperator{\OPT}{OPT}
72
+ \DeclareMathOperator{\cost}{cost}
73
+ \newcommand{\ind}{\mathbf 1}
74
+ \newcommand{\R}{\mathbb R}
75
+ \newcommand{\N}{\mathbb N}
76
+ \newcommand{\eps}{\varepsilon}
77
+ \newcommand{\abs}[1]{\lvert#1\rvert}
78
+ \newcommand{\norm}[1]{\lVert#1\rVert}
79
+ \setlist[itemize]{topsep=4pt,itemsep=3pt}
80
+ \setlist[enumerate]{topsep=4pt,itemsep=3pt}
81
+ \setlength{\emergencystretch}{2em}
82
+ \numberwithin{equation}{section}
83
+
84
+ \title{The approximation threshold for metric \(k\)-median}
85
+ \author{OpenAI}
86
+ \date{September 24, 2026}
87
+ \begin{document}
88
+ \maketitle
89
+
90
+ \begin{abstract}
91
+ For every fixed \(\varepsilon>0\), we give a deterministic polynomial-time
92
+ \((1+2/e+\varepsilon)\)-approximation for finite rational metric
93
+ \(k\)-median with specified candidate facilities, opening at most \(k\)
94
+ facilities. Under \(P\ne NP\), the infimum approximation factor in this
95
+ model is therefore \(1+2/e\).
96
+ \end{abstract}
97
+
98
+ \input{sections/introduction}
99
+ \input{sections/preliminaries}
100
+ \input{sections/preparation}
101
+ \input{sections/inequality}
102
+ \input{sections/rounding}
103
+ \input{sections/derandomization}
104
+ \appendix
105
+ \input{sections/certificates}
106
+
107
+ \bibliographystyle{plainnat}
108
+ \bibliography{references}
109
+ \end{document}
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/references.bib ADDED
@@ -0,0 +1,217 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ @inproceedings{AnandLee2024,
2
+ author = {Anand, Aditya and Lee, Euiwoong},
3
+ title = {Separating {$k$}-Median from the Supplier Version},
4
+ editor = {Vygen, Jens and Byrka, Jaros{\l}aw},
5
+ booktitle = {Integer Programming and Combinatorial Optimization: 25th International Conference, IPCO 2024},
6
+ series = {Lecture Notes in Computer Science},
7
+ volume = {14679},
8
+ pages = {14--27},
9
+ publisher = {Springer},
10
+ address = {Cham},
11
+ year = {2024},
12
+ doi = {10.1007/978-3-031-59835-7_2},
13
+ url = {https://doi.org/10.1007/978-3-031-59835-7_2},
14
+ note = {Full preprint: arXiv:2401.13819v1, January 24, 2024; \url{https://arxiv.org/abs/2401.13819v1}}
15
+ }
16
+
17
+ @article{Arya2004,
18
+ author = {Arya, Vijay and Garg, Naveen and Khandekar, Rohit and Meyerson, Adam and Munagala, Kamesh and Pandit, Vinayaka},
19
+ title = {Local Search Heuristics for {$k$}-Median and Facility Location Problems},
20
+ journal = {SIAM Journal on Computing},
21
+ volume = {33},
22
+ number = {3},
23
+ pages = {544--562},
24
+ year = {2004},
25
+ doi = {10.1137/S0097539702416402},
26
+ url = {https://doi.org/10.1137/S0097539702416402}
27
+ }
28
+
29
+ @misc{BayerTeichmann2005,
30
+ author = {Bayer, Christian and Teichmann, Josef},
31
+ title = {The Proof of {Tchakaloff}'s Theorem},
32
+ year = {2005},
33
+ eprint = {math/0502473v2},
34
+ archivePrefix = {arXiv},
35
+ primaryClass = {math.NA},
36
+ url = {https://arxiv.org/abs/math/0502473v2},
37
+ note = {Version 2, 4 May 2005; published in Proceedings of the American Mathematical Society 134(10), 3035--3040 (2006), doi:10.1090/S0002-9939-06-08249-9}
38
+ }
39
+
40
+ @article{ByrkaEtAl2017,
41
+ author = {Byrka, Jaros{\l}aw and Pensyl, Thomas and Rybicki, Bartosz and Srinivasan, Aravind and Trinh, Khoa},
42
+ title = {An Improved Approximation for {$k$}-Median and Positive Correlation in Budgeted Optimization},
43
+ journal = {ACM Transactions on Algorithms},
44
+ volume = {13},
45
+ number = {2},
46
+ articleno = {23},
47
+ pages = {23:1--23:31},
48
+ year = {2017},
49
+ doi = {10.1145/2981561},
50
+ url = {https://doi.org/10.1145/2981561},
51
+ note = {Corrected full manuscript: arXiv:1406.2951v4, 23 April 2016}
52
+ }
53
+
54
+ @misc{ByrkaEtAl2026,
55
+ author = {Byrka, Jaros{\l}aw and Guo, Yuhao and Hu, Yang and Li, Shi and Wan, Chengzhang and Wang, Zaixuan},
56
+ title = {{$k$}-Clustering via Iterative Randomized Rounding},
57
+ year = {2026},
58
+ eprint = {2604.06046v1},
59
+ archivePrefix = {arXiv},
60
+ primaryClass = {cs.DS},
61
+ doi = {10.48550/arXiv.2604.06046},
62
+ url = {https://arxiv.org/abs/2604.06046v1},
63
+ note = {Version 1, April 7, 2026}
64
+ }
65
+
66
+ @article{CGLSS2026,
67
+ author = {Cohen-Addad, Vincent and Grandoni, Fabrizio and Lee, Euiwoong and Schwiegelshohn, Chris and Svensson, Ola},
68
+ title = {A {$(2+\varepsilon)$}-Approximation Algorithm for Metric {$k$}-Median},
69
+ journal = {SIAM Journal on Computing},
70
+ year = {2026},
71
+ doi = {10.1137/25M181026X},
72
+ url = {https://doi.org/10.1137/25M181026X},
73
+ note = {Published online August 24, 2026. Full preprint: arXiv:2503.10972v2, May 19, 2026; \url{https://arxiv.org/abs/2503.10972v2}. First posted March 14, 2025}
74
+ }
75
+
76
+ @inproceedings{CharikarGuha1999,
77
+ author = {Charikar, Moses and Guha, Sudipto},
78
+ title = {Improved Combinatorial Algorithms for the Facility Location and {$k$}-Median Problems},
79
+ booktitle = {Proceedings of the 40th Annual Symposium on Foundations of Computer Science},
80
+ pages = {378--388},
81
+ year = {1999},
82
+ publisher = {IEEE Computer Society},
83
+ doi = {10.1109/SFFCS.1999.814609},
84
+ url = {https://doi.org/10.1109/SFFCS.1999.814609}
85
+ }
86
+
87
+ @article{CharikarGuhaTardosShmoys2002,
88
+ author = {Charikar, Moses and Guha, Sudipto and Tardos, {\'E}va and Shmoys, David B.},
89
+ title = {A Constant-Factor Approximation Algorithm for the {$k$}-Median Problem},
90
+ journal = {Journal of Computer and System Sciences},
91
+ volume = {65},
92
+ number = {1},
93
+ pages = {129--149},
94
+ year = {2002},
95
+ doi = {10.1006/jcss.2002.1882},
96
+ url = {https://doi.org/10.1006/jcss.2002.1882},
97
+ note = {Preliminary version in STOC 1999}
98
+ }
99
+
100
+ @inproceedings{CharikarLi2012,
101
+ author = {Charikar, Moses and Li, Shi},
102
+ title = {A Dependent {LP}-Rounding Approach for the {$k$}-Median Problem},
103
+ booktitle = {Automata, Languages, and Programming},
104
+ series = {Lecture Notes in Computer Science},
105
+ volume = {7391},
106
+ pages = {194--205},
107
+ publisher = {Springer},
108
+ year = {2012},
109
+ doi = {10.1007/978-3-642-31594-7_17},
110
+ url = {https://doi.org/10.1007/978-3-642-31594-7_17}
111
+ }
112
+
113
+ @article{Feige1998,
114
+ author = {Feige, Uriel},
115
+ title = {A Threshold of {$\ln n$} for Approximating Set Cover},
116
+ journal = {Journal of the ACM},
117
+ volume = {45},
118
+ number = {4},
119
+ pages = {634--652},
120
+ month = jul,
121
+ year = {1998},
122
+ doi = {10.1145/285055.285059},
123
+ url = {https://doi.org/10.1145/285055.285059}
124
+ }
125
+
126
+ @article{GandhiEtAl2006,
127
+ author = {Gandhi, Rajiv and Khuller, Samir and Parthasarathy, Srinivasan and Srinivasan, Aravind},
128
+ title = {Dependent Rounding and Its Applications to Approximation Algorithms},
129
+ journal = {Journal of the ACM},
130
+ volume = {53},
131
+ number = {3},
132
+ pages = {324--360},
133
+ year = {2006},
134
+ doi = {10.1145/1147954.1147956},
135
+ url = {https://doi.org/10.1145/1147954.1147956}
136
+ }
137
+
138
+ @inproceedings{GowdaEtAl2023,
139
+ author = {Gowda, Kishen N. and Pensyl, Thomas and Srinivasan, Aravind and Trinh, Khoa},
140
+ title = {Improved Bi-point Rounding Algorithms and a Golden Barrier for {$k$}-Median},
141
+ booktitle = {Proceedings of the 2023 Annual ACM-SIAM Symposium on Discrete Algorithms (SODA)},
142
+ pages = {987--1011},
143
+ publisher = {Society for Industrial and Applied Mathematics},
144
+ year = {2023},
145
+ doi = {10.1137/1.9781611977554.ch38},
146
+ url = {https://doi.org/10.1137/1.9781611977554.ch38},
147
+ note = {Preprint: \url{https://arxiv.org/abs/2210.13395v1}}
148
+ }
149
+
150
+ @article{JainEtAl2003,
151
+ author = {Jain, Kamal and Mahdian, Mohammad and Markakis, Evangelos and Saberi, Amin and Vazirani, Vijay V.},
152
+ title = {Greedy Facility Location Algorithms Analyzed Using Dual Fitting with Factor-Revealing {LP}},
153
+ journal = {Journal of the ACM},
154
+ volume = {50},
155
+ number = {6},
156
+ pages = {795--824},
157
+ year = {2003},
158
+ doi = {10.1145/950620.950621},
159
+ url = {https://doi.org/10.1145/950620.950621},
160
+ note = {Preprint: \url{https://arxiv.org/abs/cs/0207028v1}}
161
+ }
162
+
163
+ @article{JainVazirani2001,
164
+ author = {Jain, Kamal and Vazirani, Vijay V.},
165
+ title = {Approximation Algorithms for Metric Facility Location and {$k$}-Median Problems Using the Primal-Dual Schema and Lagrangian Relaxation},
166
+ journal = {Journal of the ACM},
167
+ volume = {48},
168
+ number = {2},
169
+ pages = {274--296},
170
+ year = {2001},
171
+ doi = {10.1145/375827.375845},
172
+ url = {https://doi.org/10.1145/375827.375845}
173
+ }
174
+
175
+ @article{LiSvensson2016,
176
+ author = {Li, Shi and Svensson, Ola},
177
+ title = {Approximating {$k$}-Median via Pseudo-Approximation},
178
+ journal = {SIAM Journal on Computing},
179
+ volume = {45},
180
+ number = {2},
181
+ pages = {530--547},
182
+ year = {2016},
183
+ doi = {10.1137/130938645},
184
+ url = {https://doi.org/10.1137/130938645},
185
+ note = {Author manuscript dated September 11, 2014: \url{https://tcs.nju.edu.cn/shili/papers/KM-SIMPCOMP2016.pdf}; the additive-to-ordinary reduction is Theorem 4 in that version}
186
+ }
187
+
188
+ @misc{OpenAIRecovery2026,
189
+ author = {{OpenAI}},
190
+ title = {{Single-exponential recovery and bounded-price strictness for metric $k$-median}},
191
+ howpublished = {OpenAI Math Release preprint
192
+ \href{https://github.com/openai/math/blob/main/preprints/Single-Exponential-Recovery-and-Bounded-Price-Strictness-for-Metric-k-Median-September-24-2026/paper.pdf}{OAI:Single-Exponential-Recovery-and-Bounded-Price-Strictness-for-Metric-k-Median-September-24-2026}},
193
+ year = {2026}
194
+ }
195
+
196
+ @inproceedings{Srinivasan2001,
197
+ author = {Srinivasan, Aravind},
198
+ title = {Distributions on Level-Sets with Applications to Approximation Algorithms},
199
+ booktitle = {Proceedings of the 42nd IEEE Symposium on Foundations of Computer Science},
200
+ pages = {588--597},
201
+ publisher = {IEEE Computer Society},
202
+ year = {2001},
203
+ doi = {10.1109/SFCS.2001.959935},
204
+ url = {https://doi.org/10.1109/SFCS.2001.959935}
205
+ }
206
+
207
+ @article{BBLM2005,
208
+ author = {Boucheron, St{\'e}phane and Bousquet, Olivier and Lugosi, G{\'a}bor and Massart, Pascal},
209
+ title = {Moment inequalities for functions of independent random variables},
210
+ journal = {The Annals of Probability},
211
+ volume = {33},
212
+ number = {2},
213
+ pages = {514--560},
214
+ year = {2005},
215
+ doi = {10.1214/009117904000000856},
216
+ url = {https://arxiv.org/abs/math/0503651}
217
+ }
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/certificates.tex ADDED
@@ -0,0 +1,631 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Exact certificates for the scalar bounds}
2
+ \label{app:certificates}
3
+
4
+ This appendix proves Lemma~\ref{lem:scalar-bounds}. All terminating
5
+ decimals in this appendix denote exact rational numbers. The argument
6
+ uses two finite tables of rational polynomial minorants. We give the
7
+ coefficient rule and the Bernstein conversion formula explicitly, so the
8
+ tables can be verified using only rational arithmetic; the accompanying
9
+ programs are supplementary implementations of these formulas.
10
+
11
+ Throughout, $X=1-x$, $0\le x\le1$, $0\le w\le X$, $0\le r\le1$, and
12
+ $s\in\{0,1\}$. We recall the notation
13
+ \begin{align*}
14
+ P&=\int_0^1t e^{-tx}\,dt,&
15
+ A&=3-2\int_0^1e^{-tx}\,dt,&
16
+ m&=A-1-2Px,\\
17
+ C&=1-sP,& a&=A+2Pw,& b&=(2-s)P(x+w),\qquad z=Pw^2,\\
18
+ k_s&=(1-s)\frac{1-\sqrt{1-P}}{1+\sqrt{1-P}},&
19
+ K&=C-k_s-br+1.6z,\\
20
+ L&=(C-m-b)r+.4z,&
21
+ M&=(1-r)a+CPr,& G&=M-L.
22
+ \end{align*}
23
+ Also set
24
+ \[
25
+ d_0=.52,\qquad d_1=.4,\qquad
26
+ H_0=.394-.42X^2+.04X^3,\qquad H_1=.25,\qquad J_s=CH_s.
27
+ \]
28
+ The elementary integral bounds give $0<P\le.5$ and $1\le A\le2$;
29
+ the latter follows from $1-e^{-tx}\le tx$. Direct integration gives
30
+ \begin{equation}
31
+ (1+x)(A-1)=2x(1-P).
32
+ \label{eq:cert-integral-identity}
33
+ \end{equation}
34
+
35
+ \subsection{Rational approximations and their errors}
36
+ \label{sec:cert-interpolation}
37
+
38
+ Use the following polynomials in $X$, with coefficients displayed in
39
+ ascending order:
40
+ \begin{equation}
41
+ \begin{aligned}
42
+ p(X)={}&.26424112+.16053514X+.05751895X^2\\
43
+ &\hspace{12mm}+.01313705X^3+.00456774X^4,\\
44
+ v(X)={}&1.73575888-.52832269X-.16191093X^2\\
45
+ &\hspace{12mm}-.03442938X^3-.01109588X^4,\\
46
+ k(X)={}&.0767+.0564X+.0142X^2+.0246X^3.
47
+ \end{aligned}
48
+ \label{eq:cert-interpolants}
49
+ \end{equation}
50
+ We will prove
51
+ \begin{equation}
52
+ |p-P|\le\epsilon_P:=.0000075,\qquad
53
+ |v-A|\le2\epsilon_P=.000015,\qquad k_0\le k.
54
+ \label{eq:cert-approximation-errors}
55
+ \end{equation}
56
+
57
+ For the first two claims, the integral Taylor series are
58
+ \[
59
+ P(x)=\sum_{n\ge0}\frac{(-x)^n}{n!(n+2)},\qquad
60
+ A(x)=3-2\sum_{n\ge0}\frac{(-x)^n}{n!(n+1)}.
61
+ \]
62
+ On $0\le x\le1$ the magnitudes of the summands decrease. Thus the
63
+ partial sums through orders $12$ and $13$ enclose each defining
64
+ integral. Evaluating these rational enclosures at
65
+ $X=0,1/4,1/2,3/4,1$ proves that the nodal errors of the displayed
66
+ $p,v$ are, respectively, less than
67
+ $2.343560\cdot10^{-9}$ and $2.344324\cdot10^{-9}$. In particular,
68
+ each is less than $4\cdot10^{-9}$. This nodal calculation can be
69
+ performed without evaluating any transcendental number: at each node
70
+ substitute $x=1-X$ into the two finite sums just given and compare
71
+ both rational endpoints with the displayed polynomial value.
72
+
73
+ Let $I_P,I_A$ be the exact degree-four interpolants at these five nodes.
74
+ The sum of the absolute values of the Lagrange basis polynomials is at
75
+ most
76
+ \[
77
+ \sum_{i=0}^4\frac{4^4}{i!(4-i)!}=\frac{512}{3},
78
+ \]
79
+ because every numerator factor has absolute value at most one.
80
+ Differentiating with respect to $X$ gives the fifth-derivative bounds
81
+ $1/7$ for $P$ and $1/3$ for $A$. The absolute node product, with
82
+ $u=|X-1/2|$, is
83
+ \[
84
+ u(1/4-u^2)|1/16-u^2|.
85
+ \]
86
+ For $u\le1/4$ it is at most $1/256$. For $1/4\le u\le1/2$, the
87
+ product of the two quadratic factors is at most
88
+ $((1/4-1/16)/2)^2=9/1024$, so the entire expression is at most
89
+ $9/2048$. Both bounds are less than $.0045$. The interpolation
90
+ remainder formula therefore gives
91
+ \begin{align*}
92
+ |p-P|&\le\frac{512}{3}(4\cdot10^{-9})+\frac{.0045}{840}
93
+ =\frac{31709}{5250000000}<\epsilon_P,\\
94
+ |v-A|&\le\frac{512}{3}(4\cdot10^{-9})+\frac{.0045}{360}
95
+ =\frac{9887}{750000000}<2\epsilon_P.
96
+ \end{align*}
97
+
98
+ The coefficient signs and endpoint values give
99
+ \begin{equation}
100
+ \begin{gathered}
101
+ .26424112\le p\le.5,\qquad 1\le v\le1.73575888,\\
102
+ .0767\le k\le.1719,\qquad .014\le H_0\le.394.
103
+ \end{gathered}
104
+ \label{eq:cert-polynomial-ranges}
105
+ \end{equation}
106
+ For $H_0$, use $H_0'(X)=X(-.84+.12X)\le0$.
107
+ The first row of Table~\ref{tab:cert-first} below proves
108
+ \begin{equation}
109
+ T_k:=4k-(p+\epsilon_P)(1+k)^2>0.
110
+ \label{eq:cert-k-envelope}
111
+ \end{equation}
112
+ Since $0<k<1$ and $t\mapsto4t/(1+t)^2$ is increasing on $(0,1)$,
113
+ while $4k_0/(1+k_0)^2=P$, inequality~\eqref{eq:cert-k-envelope}
114
+ and $P\le p+\epsilon_P$ imply $k_0\le k$. This proves all of
115
+ \eqref{eq:cert-approximation-errors}.
116
+
117
+ Define polynomial versions of the quantities used in the following reductions by
118
+ \begin{equation}
119
+ \begin{gathered}
120
+ c=1-sp,\qquad N=c-(1-s)k,\qquad l=c+1-v+spx,\\
121
+ d=d_s,\qquad h=1.6+.4d,\qquad
122
+ u_0=d/h,\qquad u_1=(2-s)(1+d)/(2h).
123
+ \end{gathered}
124
+ \label{eq:cert-polynomial-notation}
125
+ \end{equation}
126
+ The polynomial families in the reductions are
127
+ \begin{align*}
128
+ T_1&=1-p-1.12p(1+x)+.4p^2X(1+x),\\
129
+ T_2&=((1-p)^2-.38pX+px)(1+x)-2x(1-p),\\
130
+ Q_0(W)&=N-dv+pW(hW-2d),\\
131
+ Q_1&=N-(2-s)px-d(cp-l)-hp u_1^2,\\
132
+ Y&=N-p\bigl((2-s)x+(2-s)^2/6.4\bigr),\\
133
+ Y'&=N+p(1.6X^2-2)\qquad(s=0).
134
+ \end{align*}
135
+ The notation $T(P,A)$ means replacement of $p,v$ by $P,A$, keeping
136
+ $X,k$ and the rational constants fixed.
137
+
138
+
139
+ \subsection{Reduction of the first, second, and final scalar bounds}
140
+
141
+ We first establish the first scalar inequality
142
+ \begin{equation}
143
+ m+b-.4z/r\le\frac{C(1-P)}{1-Pr}\qquad(0<r\le1).
144
+ \label{eq:cert-first-scalar}
145
+ \end{equation}
146
+ Put $t=1/r-P>0$. By~\eqref{eq:cert-integral-identity}, the right
147
+ side of~\eqref{eq:cert-first-scalar} minus its left side equals
148
+ \begin{align*}
149
+ &C(1-P)-\frac{2x(1-P)}{1+x}+sPx-(2-s)Pw+.4P^2w^2\\
150
+ &\hspace{35mm}+P\left(\frac{C(1-P)}t+.4w^2t\right).
151
+ \end{align*}
152
+ Applying AM--GM to the last parentheses gives the lower bound
153
+ \begin{equation}
154
+ C(1-P)-\frac{2x(1-P)}{1+x}+sPx
155
+ -(2-s-2\sqrt{.4C(1-P)})Pw+.4P^2w^2.
156
+ \label{eq:cert-amgm}
157
+ \end{equation}
158
+ For $s=0$ the coefficient $2-2\sqrt{.4(1-P)}$ is at most $1.12$.
159
+ The resulting quadratic decreases for $0\le w\le X$: its derivative
160
+ is at most $-1.12P+.8P^2<0$. Substituting $w=X$ into this lower
161
+ bound gives $X T_1(P)/(1+x)$, where $T_1$ is defined above. For
162
+ $s=1$, the coefficient $1-2\sqrt{.4}(1-P)$ is at most $.38$.
163
+ Dropping the nonnegative quadratic term and using $w\le X$ gives
164
+ $T_2(P)/(1+x)$. The numerical coefficient comparisons also follow
165
+ by squaring positive quantities: $.2>.44^2$ and
166
+ $.4>.62^2$. Table~\ref{tab:cert-first}, with the substitution
167
+ budget proved below, gives $T_1(P),T_2(P)>0$.
168
+ At $X=0$, the extra factor $X$ in the $s=0$ reduction is zero,
169
+ which still proves the required non-strict inequality.
170
+
171
+ For $r>0$, \eqref{eq:cert-first-scalar} implies
172
+ \[
173
+ L\ge Cr\left(1-\frac{1-P}{1-Pr}\right)\ge0.
174
+ \]
175
+ For $r=0$, one has $L=.4z\ge0$ directly.
176
+
177
+ To check $K\ge d_sG$, write $d=d_s$ and $h=1.6+.4d$.
178
+ The difference $K-dG$ is affine in $r$. With
179
+ $N_P=C-(1-s)k$, replacing $k_s$ by $(1-s)k$ only decreases this
180
+ difference. Put $\underline K=N_P-br+1.6z\le K$. The endpoint
181
+ expressions after this replacement are
182
+ \begin{align}
183
+ (\underline K-dG)|_{r=0}&=N_P-dA+Pw(hw-2d),
184
+ \label{eq:cert-r0}\\
185
+ (\underline K-dG)|_{r=1}&=Q_1(P,A)+hP(w-u_1)^2,
186
+ \label{eq:cert-r1}
187
+ \end{align}
188
+ where
189
+ \[
190
+ u_0=d/h,\qquad u_1=\frac{(2-s)(1+d)}{2h}
191
+ \]
192
+ and $Q_1$ is defined above. For $s=1$ we may use the unrestricted
193
+ minimum $w=u_0$ in~\eqref{eq:cert-r0}. For $s=0$, the constrained
194
+ minimum is at $w=X$ if $X\le u_0$, and at $w=u_0$ otherwise.
195
+ Equation~\eqref{eq:cert-r1} is bounded below by $Q_1(P,A)$ for
196
+ both values of $s$. These are precisely the $Q_0,Q_1$ checks in
197
+ Table~\ref{tab:cert-first}.
198
+
199
+ We next reduce the final two scalar bounds. Recall
200
+ \[
201
+ \kappa_s(q)=C\frac{1-q}{1-Pq}-(1-q),\qquad 0\le q\le1.
202
+ \]
203
+ For $s=1$, $k_s=0$ and $\kappa_s(q)\le0$. Thus both relevant
204
+ left sides are bounded below by $C+1.6z-b$. Its unrestricted
205
+ minimum in $w$ is the true-parameter version of $Y$ above, so the
206
+ rows $Y-H_0$ and $Y-.25$ suffice.
207
+
208
+ For $s=0$ and $X\ge.5$, use $q\le1$ and $\kappa_0(q)\le k_0$.
209
+ Again a common lower bound is $1-k_0+1.6z-b$, whose unrestricted
210
+ minimum is the corresponding $Y$. For $s=0$ and $X\le.5$, we
211
+ have $x\ge.5$ and
212
+ \[
213
+ P(x)\le P(.5)<.47.
214
+ \]
215
+ For example the inequality $e^{-u}\le1-u+u^2/2$ yields
216
+ $P(.5)\le1/2-1/6+1/32=35/96<.47$.
217
+ It follows that $b\ge .52P/(1-P)$, because $x+w\ge.5$ and
218
+ $1-P>.53$. Since
219
+ \[
220
+ \kappa_0(q)=\frac{Pq(1-q)}{1-Pq}
221
+ \le\frac{P}{1-P}(1-q),
222
+ \]
223
+ we obtain $bq+.52\kappa_0(q)\le b$. The fourth scalar left side
224
+ is consequently at least
225
+ \[
226
+ 1-.48k_0+1.6z-b.
227
+ \]
228
+ The quadratic $1.6Pw^2-2P(x+w)$ decreases on $0\le w\le X\le.5$,
229
+ so its minimum is $P(1.6X^2-2)$. Thus the fourth and fifth
230
+ inequalities follow, respectively, from $Y'+.52k-H_0\ge0$ and
231
+ $Y'-.25\ge0$ after substitution. In the former expression the
232
+ net coefficient of $k$ is $-.48$, so replacing $k_0$ by the upper
233
+ bound $k$ is conservative.
234
+
235
+ The last scalar bound also gives positivity of $K$: since $b\ge0$,
236
+ \[
237
+ K=C-k_s-br+1.6z\ge C-k_s-b+1.6z\ge.25>0.
238
+ \]
239
+
240
+ \subsection{The first coefficient table and its exact verification}
241
+
242
+ Replacing $p,v$ by $P,A$ in these expressions changes their values
243
+ by less than
244
+ \begin{equation}
245
+ \sigma=.0002.
246
+ \label{eq:cert-sigma}
247
+ \end{equation}
248
+ For completeness, the following derivative bounds hold on the line
249
+ segment between $(p,v)$ and $(P,A)$, using $0\le p,P\le.5$,
250
+ $1\le v,A\le2$, and $0\le W\le1$:
251
+ \[
252
+ \begin{array}{c|rr|r}
253
+ T&|\partial_pT|&|\partial_vT|&
254
+ 10^6\,|T(p,v)-T(P,A)|\text{ upper bound}\\ \hline
255
+ T_1&3.64&0&27.3\\
256
+ T_2&8.76&0&65.7\\
257
+ Q_0(W)&3.848&.52&36.66\\
258
+ Q_1&4.848&.52&44.16\\
259
+ Y&2.625&0&19.6875\\
260
+ Y'&2&0&15
261
+ \end{array}
262
+ \]
263
+ Here $T_{1,p}=-1-1.12(1+x)+.8pX(1+x)$, with
264
+ $X(1+x)\le1$, and
265
+ $T_{2,p}=[-2(1-p)-.38X+x](1+x)+2x$.
266
+ For $Q_0$, use $h\le1.808$ and $2d\le1.04$.
267
+ For $Q_1$, $(cp-l)_p=1-2sp+sX$ has absolute value at most $2$,
268
+ $(cp-l)_v=1$, and $u_1\le1$.
269
+ The last two derivative bounds follow directly from their displayed
270
+ linear dependence on $p$. These estimates prove the claimed budget
271
+ even on the full interval, rather than only the listed subintervals.
272
+ Adding $.52k$ or subtracting $H_0,.25$ does not change this budget.
273
+ The row for $T_k$ already includes $\epsilon_P$ explicitly and does
274
+ not need this additional substitution estimate.
275
+
276
+ Here is the finite verification mechanism used in both coefficient
277
+ tables. A row with scale $10^a$ and integers
278
+ $\lambda_0,\ldots,\lambda_n$ asserts
279
+ \begin{equation}
280
+ T(X)\ge t(X):=10^{-a}\sum_{j=0}^n\lambda_jX^j
281
+ \qquad(0\le X\le1).
282
+ \label{eq:cert-minorant}
283
+ \end{equation}
284
+ To verify it, expand $T=\sum_jc_jX^j$ and check
285
+ \begin{equation}
286
+ 10^ac_j\ge\lambda_j\quad(0\le j<n),\qquad
287
+ 10^a\sum_{j\ge n}\min(0,c_j)\ge\lambda_n.
288
+ \label{eq:cert-coefficient-rule}
289
+ \end{equation}
290
+ Positive tail terms may be discarded; for every negative tail term,
291
+ $c_jX^j\ge c_jX^n$. This proves~\eqref{eq:cert-minorant}.
292
+
293
+ All short minorants have degree at most six. On any listed interval
294
+ $[\alpha,\beta]$, their degree-six Bernstein coefficients are
295
+ \begin{equation}
296
+ \mathfrak b_m(t;\alpha,\beta)=10^{-a}
297
+ \sum_{h=0}^m\frac{\binom mh}{\binom6h}(\beta-\alpha)^h
298
+ \sum_{j=h}^n\lambda_j\binom jh\alpha^{j-h},
299
+ \quad 0\le m\le6.
300
+ \label{eq:cert-bernstein-rule}
301
+ \end{equation}
302
+ Indeed, expand at $X=\alpha+(\beta-\alpha)u$ and convert ordinary
303
+ powers of $u$ to degree-six Bernstein form. Thus if every coefficient
304
+ in~\eqref{eq:cert-bernstein-rule} is at least $b_*$, then
305
+ $t(X)\ge b_*$ throughout the interval, since the Bernstein basis is
306
+ nonnegative and sums to one. An endpoints entry with more than two
307
+ numbers prescribes each interval between consecutive numbers.
308
+
309
+ \begingroup
310
+ \small
311
+ \setlength{\tabcolsep}{3pt}
312
+ \renewcommand{\arraystretch}{1.18}
313
+ \begin{longtable}{@{}lclc>{\raggedright\arraybackslash}p{.39\textwidth}@{}}
314
+ \caption{First coefficient table. The scale is $10^a$, and the
315
+ listed vector is $(\lambda_0,\ldots,\lambda_n)$.}
316
+ \label{tab:cert-first}\\
317
+ \toprule
318
+ $T$&$s$&Endpoints and splits&$a$&$\lambda$\\
319
+ \midrule
320
+ \endfirsthead
321
+ \toprule
322
+ $T$&$s$&Endpoints and splits&$a$&$\lambda$\\
323
+ \midrule
324
+ \endhead
325
+ \bottomrule
326
+ \endfoot
327
+ $T_k$&--&$0,.5,1$&4&$(4,73,-384,563,-184,-67)$\\
328
+ $T_1$&--&$0,1$&2&$(14,-17,3,3,-1)$\\
329
+ $T_2$&--&$0,1$&2&$(13,10,-22)$\\
330
+ $Q_0(u_0)$&1&$0,1$&2&$(1,3,-1)$\\
331
+ $Q_1$&1&$0,1$&2&$(42,-3)$\\
332
+ $Q_1$&0&$0,1$&2&$(5,-1)$\\
333
+ $Q_0(u_0)$&0&$u_0,1$&2&$(-2,19,-1)$\\
334
+ $Q_0(X)$&0&$0,u_0$&2&$(2,-6)$\\
335
+ $Y-H_0$&1&$0,1$&2&$(3,-9,45,-2)$\\
336
+ $Y-.25$&1&$0,1$&2&$(17,-9)$\\
337
+ $Y-H_0$&0&$.5,1$&3&$(-165,50,575,-1)$\\
338
+ $Y-.25$&0&$.5,1$&2&$(-3,5,15,-1)$\\
339
+ $Y'+.52k-H_0$&0&$0,.125,.25,.5$&4&$(406,-3483,7208,1786,-3)$\\
340
+ $Y'-.25$&0&$0,.5$&2&$(14,-38,29,-1)$\\
341
+ \end{longtable}
342
+ \endgroup
343
+
344
+ Substitution of~\eqref{eq:cert-interpolants} into the definitions
345
+ verifies~\eqref{eq:cert-coefficient-rule} for all fourteen rows of
346
+ Table~\ref{tab:cert-first}. As additional explicit sign certificates,
347
+ the minima of the finite sets in~\eqref{eq:cert-bernstein-rule}, over
348
+ all prescribed subintervals for each row, are at least $10^{-6}$ times
349
+ the following integers, in row order:
350
+ \begin{equation}
351
+ \begin{gathered}
352
+ 114, 20000, 10000, 10000, 390000, 40000, 33818,\\
353
+ 2743, 15000, 80000, 3625, 31250, 356, 21250.
354
+ \end{gathered}
355
+ \label{eq:cert-first-bernstein-lower}
356
+ \end{equation}
357
+ Both~\eqref{eq:cert-coefficient-rule} and these lower bounds are finite
358
+ rational comparisons specified completely by the table and
359
+ \eqref{eq:cert-bernstein-rule}. For example, the first row has
360
+ smallest Bernstein coefficient $73/640000$, and the thirteenth row
361
+ has smallest coefficient $27341/76800000$.
362
+ Consequently $T_k>0$, and every other short minorant exceeds
363
+ $\sigma=.0002$ on its indicated intervals. After the substitution
364
+ budget, this completes the first and second groups of scalar bounds
365
+ and the final two scalar bounds.
366
+
367
+ \subsection{The third scalar bound: perturbation estimate}
368
+
369
+ It remains to prove
370
+ \begin{equation}
371
+ ((J_s-b)r+1.6z)M+(C-k_s-J_sr)L\ge0.
372
+ \label{eq:cert-third-goal}
373
+ \end{equation}
374
+ Since $L\ge0$ is already established, replacing $k_s$ with $(1-s)k$
375
+ only decreases the left side. We next replace $P,A$ by $p,v$.
376
+ This replacement changes the expression by at most
377
+ \begin{equation}
378
+ \sigma(r+w^2),\qquad \sigma=.0002.
379
+ \label{eq:cert-third-error}
380
+ \end{equation}
381
+ Here are full bounds for this assertion. For either endpoint choice
382
+ $(\pi,\nu)=(P,A)$ or $(p,v)$, put $c_\pi=1-s\pi$, $H=H_s$, and
383
+ write the two products as $F_1F_2+F_3F_4$, where
384
+ \begin{align*}
385
+ F_1&=[c_\pi H-(2-s)\pi(x+w)]r+1.6\pi w^2,\\
386
+ F_2&=(1-r)(\nu+2\pi w)+c_\pi\pi r,\\
387
+ F_3&=c_\pi(1-Hr)-(1-s)k,\\
388
+ F_4&=[2-\nu-s\pi X-(2-s)\pi w]r+.4\pi w^2.
389
+ \end{align*}
390
+ Writing $\rho=r+w^2$, the ranges already established imply
391
+ \begin{equation}
392
+ |F_1|\le1.1\rho,\qquad |F_2|\le3,\qquad
393
+ |F_3|\le1,\qquad |F_4|\le2\rho.
394
+ \label{eq:cert-factor-bounds}
395
+ \end{equation}
396
+ For $F_1$, both nonnegative terms in its coefficient of $r$ are at
397
+ most one, while $1.6\pi\le.8$. The expression $F_2$ is a convex
398
+ combination of two quantities between zero and three. For $F_3$,
399
+ the lower bounds are $1-.394-.1719=.4341$ when $s=0$ and
400
+ $.5(1-.25)=.375$ when $s=1$, and the upper bound is one.
401
+ Finally the coefficient of $r$ in $F_4$ belongs to $[-1,1]$:
402
+ $0\le2-\nu\le1$ and $0\le s\pi X+(2-s)\pi w\le1$.
403
+
404
+ Let $\delta F_j$ denote the change between the two choices. With
405
+ $\epsilon_P=.0000075$, direct subtraction gives
406
+ \begin{align*}
407
+ |\delta F_1|&\le2\epsilon_P\rho,&
408
+ |\delta F_2|&\le4\epsilon_P,\\
409
+ |\delta F_3|&\le\epsilon_P,&
410
+ |\delta F_4|&\le4\epsilon_P\rho.
411
+ \end{align*}
412
+ For the first estimate, the coefficient multiplying
413
+ $\epsilon_Pr$ is $sH+(2-s)(x+w)$, at most $2$ for $s=0$ and at
414
+ most $1.25$ for $s=1$; the remaining coefficient is $1.6$.
415
+ For the second, use the convex combination in $r$, together with
416
+ $|\delta(\nu+2\pi w)|\le4\epsilon_P$ and
417
+ \[
418
+ |\delta(c_\pi\pi)|
419
+ =|P-p|\,|1-s(P+p)|\le\epsilon_P.
420
+ \]
421
+ The third estimate is immediate from $0\le1-Hr\le1$.
422
+ For the fourth, use
423
+ $2+sX+(2-s)w\le4$ and $.4\le4$.
424
+ Combining these differences with~\eqref{eq:cert-factor-bounds} and
425
+ the identity $ab-a'b'=(a-a')b+a'(b-b')$ yields
426
+ \begin{align*}
427
+ |\delta(F_1F_2+F_3F_4)|
428
+ &\le(3\cdot15+1.1\cdot30+2\cdot7.5+30)10^{-6}\rho\\
429
+ &=.000123\rho<\sigma\rho\qquad(\rho>0).
430
+ \end{align*}
431
+ If $\rho=0$, both expressions vanish. Thus
432
+ \eqref{eq:cert-third-error} holds throughout the domain. The factor
433
+ bounds hold for both choices, so this telescoping estimate already
434
+ accounts for products of perturbations.
435
+
436
+ \subsection{Bernstein expansion and the second coefficient table}
437
+
438
+ Use the polynomial quantities in~\eqref{eq:cert-polynomial-notation},
439
+ and set
440
+ \[
441
+ j=cH_s,\qquad b'_0=(2-s)px,\qquad b'_1=(2-s)pX,
442
+ \qquad f=2pX,\qquad Z'=pX^2.
443
+ \]
444
+ In the polynomial version of the left side of
445
+ \eqref{eq:cert-third-goal}, subtract $\sigma(r+w^2)$ and put
446
+ $w=X\eta$, $0\le\eta\le1$. Its degree-three Bernstein
447
+ coefficients in $\eta$, for $i=0,1,2,3$, are
448
+ \begin{equation}
449
+ B_0+B_1r+B_2r^2,
450
+ \label{eq:cert-eta-coefficient}
451
+ \end{equation}
452
+ where, writing $e=i/3$, $e_2=i(i-1)/6$, and
453
+ $t=\mathbf{1}_{\{i=3\}}$, the exact formulas are
454
+ \begin{equation}
455
+ \begin{aligned}
456
+ B_0={}&Z'\bigl((1.6v+.4N)e_2+1.6ft\bigr)-\sigma X^2e_2,\\
457
+ B_1={}&(j-b'_0)v+Nl\\
458
+ &+\bigl((j-b'_0)f-b'_1v-Nb'_1\bigr)e-b'_1fe_2\\
459
+ &-Z'\bigl((1.6(v-cp)+.4j)e_2+1.6ft\bigr)-\sigma,\\
460
+ B_2={}&(b'_0-j)(v-cp)-jl\\
461
+ &+\bigl((b'_0-j)f+b'_1(v-cp)+jb'_1\bigr)e+b'_1fe_2.
462
+ \end{aligned}
463
+ \label{eq:cert-bcoeff}
464
+ \end{equation}
465
+ These formulas give all eight expansions, one for each pair $(s,i)$.
466
+ They can also be derived directly by expanding
467
+ \begin{align*}
468
+ &\bigl([j-(2-s)p(x+w)]r+1.6pw^2\bigr)
469
+ \bigl((1-r)(v+2pw)+cpr\bigr)\\
470
+ &\quad +(N-jr)\bigl([l-(2-s)pw]r+.4pw^2\bigr)
471
+ -\sigma(r+w^2)
472
+ \end{align*}
473
+ in powers of $\eta$ after $w=X\eta$, and using the degree-three
474
+ conversion rule: if $a_h$ is the coefficient of $\eta^h$, the
475
+ $i$th Bernstein coefficient is
476
+ $\sum_{h=0}^i a_h\binom ih/\binom3h$.
477
+
478
+ In all eight cases $B_0\ge0$. For $i=0,1$, it is zero. Otherwise
479
+ \[
480
+ B_0=X^2\bigl(p(1.6v+.4N)-\sigma\bigr)e_2+1.6pX^2ft.
481
+ \]
482
+ Here $N\ge.5$, $v\ge1$, and $p\ge.26424112$, so the bracket is
483
+ at least $.475434016>0$ and the other term is nonnegative.
484
+
485
+ Define
486
+ \[
487
+ D'=4B_0B_2-B_1^2,\qquad S'=B_0+B_1+B_2.
488
+ \]
489
+ For $i\le1$, positivity of $B_1$ and $B_1+B_2$ proves
490
+ nonnegativity of~\eqref{eq:cert-eta-coefficient} on $0\le r\le1$.
491
+ For $i\ge2$, any of the following is sufficient:
492
+ \begin{enumerate}
493
+ \item $B_1,B_2\ge0$;
494
+ \item $D'>0$;
495
+ \item $S'>0$ and $B_0-B_2>0$.
496
+ \end{enumerate}
497
+ For the second criterion, $B_0\ge0$ and $D'>0$ force
498
+ $B_0,B_2>0$; completing the square proves positivity for every
499
+ real $r$. For the third, use
500
+ \[
501
+ B_0+B_1r+B_2r^2
502
+ =rS'+(1-r)(B_0-rB_2),
503
+ \]
504
+ where $B_0-rB_2=(1-r)B_0+r(B_0-B_2)\ge0$.
505
+
506
+ Table~\ref{tab:cert-third} supplies these signs. It uses exactly
507
+ the coefficient rule~\eqref{eq:cert-coefficient-rule} and the
508
+ degree-six Bernstein formula~\eqref{eq:cert-bernstein-rule}.
509
+
510
+ \begingroup
511
+ \small
512
+ \setlength{\tabcolsep}{3pt}
513
+ \renewcommand{\arraystretch}{1.18}
514
+ \begin{longtable}{@{}ccllc>{\raggedright\arraybackslash}p{.38\textwidth}@{}}
515
+ \caption{Second coefficient table. A row with $i=0,1$ supplies
516
+ the indicated certificate separately for both values of $i$.}
517
+ \label{tab:cert-third}\\
518
+ \toprule
519
+ $s$&$i$&Endpoints and splits&$T$&$a$&$\lambda$\\
520
+ \midrule
521
+ \endfirsthead
522
+ \toprule
523
+ $s$&$i$&Endpoints and splits&$T$&$a$&$\lambda$\\
524
+ \midrule
525
+ \endhead
526
+ \bottomrule
527
+ \endfoot
528
+ 0&0&$0,1$&$B_1$&2&$(1,90,-39)$\\
529
+ 0&1&$0,1$&$B_1$&2&$(1,41,-51,28,-1)$\\
530
+ 0&$0,1$&$0,1$&$B_1+B_2$&2&$(10,-1)$\\
531
+ 0&2&$0,.05$&$B_1$&2&$(1,-9,-98)$\\
532
+ 0&2&$0,.05$&$B_2$&2&$(9,-23)$\\
533
+ 0&2&$.05,1$&$D'$&4&$\begin{gathered}(-2,16,1176,-153,\\-1500,2590,-1000)\end{gathered}$\\
534
+ 0&3&$0,.015$&$B_1$&2&$(1,-58,-262)$\\
535
+ 0&3&$0,.015$&$B_2$&2&$(9,-5)$\\
536
+ 0&3&$.015,.25,.5,1$&$D'$&5&$\begin{gathered}(-12,1180,2070,-32420,\\44210,33740,-14000)\end{gathered}$\\
537
+ 1&0&$0,1$&$B_1$&2&$(5,30,-7)$\\
538
+ 1&0&$0,1$&$B_1+B_2$&2&$(12,-4)$\\
539
+ 1&1&$0,1$&$B_1$&2&$(5,-1)$\\
540
+ 1&1&$0,1$&$B_1+B_2$&2&$(12,-8)$\\
541
+ 1&2&$0,.2$&$B_1$&2&$(5,-16,-41)$\\
542
+ 1&2&$0,.2$&$B_2$&2&$(7,-2)$\\
543
+ 1&2&$.2,1$&$D'$&3&$(-4,17,92,87,-135)$\\
544
+ 1&3&$0,.1$&$B_1$&3&$(54,-391,-941,-900)$\\
545
+ 1&3&$0,.1$&$B_2$&2&$(7,-1)$\\
546
+ 1&3&$.1,.75$&$D'$&3&$(-4,42,194,478,-995)$\\
547
+ 1&3&$.75,1$&$S'$&2&$(12,-9)$\\
548
+ 1&3&$.75,1$&$B_0-B_2$&2&$(-8,-32,67,-1)$\\
549
+ \end{longtable}
550
+ \endgroup
551
+
552
+ In the printed row order, the Bernstein coefficients of these short
553
+ minorants, over all of each row's subintervals, are at least
554
+ $10^{-6}$ times the following integers:
555
+ \begin{equation}
556
+ \begin{gathered}
557
+ 10000, 10000, 90000, 3050, 78500, 171, 710,\\
558
+ 89250, 60, 50000, 80000, 40000, 40000, 1600,\\
559
+ 66000, 3560, 4590, 69000, 2518, 30000, 52656.
560
+ \end{gathered}
561
+ \label{eq:cert-third-bernstein-lower}
562
+ \end{equation}
563
+ The bound $90000$ in the third position applies to both indices in
564
+ that row. These are all positive. The smallest exact Bernstein
565
+ coefficient among the table's checks is
566
+ $193875074979/3200000000000000$, in the ninth printed row.
567
+ Thus all the required strict signs follow from the finite rational
568
+ formula~\eqref{eq:cert-bernstein-rule}.
569
+
570
+ For clarity, the negative-tail calculations needed for the four
571
+ discriminant rows are detailed next. Let
572
+ $b_{h,j}=[X^j]B_h$ and write
573
+ \[
574
+ c_j=[X^j]D'
575
+ =\sum_u\bigl(4b_{0,u}b_{2,j-u}-b_{1,u}b_{1,j-u}\bigr),
576
+ \]
577
+ where coefficients outside the degree range are zero. For a short
578
+ minorant of degree $n$, group $\min(0,c_j)$ in consecutive blocks
579
+ of five starting at $j=n$, truncating at degree $28$. The five block
580
+ sums are bounded below by $.0001$ times the following integers:
581
+ \begin{equation}
582
+ \begin{array}{cc|c|c|rrrrr}
583
+ s&i&n&\deg D'&1&2&3&4&5\\ \hline
584
+ 0&2&6&20&-930&-11&-1&0&0\\
585
+ 0&3&6&22&-1070&-180&-2&-1&0\\
586
+ 1&2&4&28&-1312&-18&-1&-1&-1\\
587
+ 1&3&4&28&-8240&-1560&-29&-1&-1
588
+ \end{array}
589
+ \label{eq:cert-tail-blocks}
590
+ \end{equation}
591
+ These twenty rational comparisons follow by substituting
592
+ \eqref{eq:cert-bcoeff} and~\eqref{eq:cert-interpolants} into the
593
+ displayed coefficient formula. Their row sums are, respectively,
594
+ $-.0942,-.1253,-.1333,-.9831$, which are at least the final scaled
595
+ minorant coefficients $-.1,-.14,-.135,-.995$.
596
+ For all entries before the last, one checks simply
597
+ $10^a[X^j]T\ge\lambda_j$ as in
598
+ \eqref{eq:cert-coefficient-rule}. The same coefficient rule verifies
599
+ the non-discriminant rows directly.
600
+
601
+ The tail cutoff is exact: the four discriminant degrees are
602
+ $20,22,28,28$, as recorded in~\eqref{eq:cert-tail-blocks}, so no
603
+ term above degree $28$ has been omitted. More generally, from
604
+ \eqref{eq:cert-bcoeff}, the respective triples of degrees
605
+ $(\deg B_0,\deg B_1,\deg B_2)$ are
606
+ \[
607
+ \begin{array}{c|rrrr}
608
+ &i=0&i=1&i=2&i=3\\ \hline
609
+ s=0&(-\infty,9,9)&(-\infty,10,10)&(10,10,10)&(11,11,9)\\
610
+ s=1&(-\infty,9,13)&(-\infty,10,13)&(10,14,13)&(11,14,12).
611
+ \end{array}
612
+ \]
613
+ Here $\deg0=-\infty$. These bounds also justify a uniform cutoff of
614
+ $28$ for every polynomial in the two coefficient tables.
615
+
616
+ For $(s,i)=(0,2)$, the first criterion covers $X\in[0,.05]$ and
617
+ the discriminant criterion covers $X\in[.05,1]$.
618
+ For $(s,i)=(0,3)$, the corresponding split is $.015$, with the
619
+ listed additional subdivisions used only for Bernstein positivity.
620
+ For $(s,i)=(1,2)$, the split is $.2$.
621
+ For $(s,i)=(1,3)$, the first criterion covers $[0,.1]$, the
622
+ discriminant criterion covers $[.1,.75]$, and the final criterion
623
+ covers $[.75,1]$. For $i=0,1$, the full interval is covered by
624
+ $B_1$ and $B_1+B_2$. All endpoints belong to the stated intervals.
625
+ Thus every coefficient~\eqref{eq:cert-eta-coefficient} is nonnegative
626
+ for $0\le X,r\le1$. Nonnegativity and unit sum of the degree-three
627
+ Bernstein basis in $\eta$ prove the desired polynomial inequality
628
+ for $0\le w\le X$; when $X=0$ one has $w=0$ directly.
629
+ Restoring the error budget~\eqref{eq:cert-third-error} proves
630
+ \eqref{eq:cert-third-goal}. Together with the preceding reductions,
631
+ this completes the proof of Lemma~\ref{lem:scalar-bounds}.
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/derandomization.tex ADDED
@@ -0,0 +1,585 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Deterministic implementation and completion}
2
+ \label{sec:derandomization}
3
+
4
+ The preceding constructions yield an additive approximation in expectation.
5
+ We now replace their random choices by finite distributions of polynomial
6
+ support, and then choose the least expensive feasible outcome. Throughout
7
+ this section the desired approximation loss is fixed. In particular, the
8
+ grid denominator, the number of physical rounds, and all parameters chosen
9
+ in Theorems~\ref{thm:preparation} and~\ref{thm:grid-rounding} are constants
10
+ independent of the input size. All input distances are rational, and
11
+ running time includes their encoding lengths.
12
+
13
+ \subsection{Compression of finite distributions}
14
+
15
+ A distribution list is a finite list of states, each equipped with a
16
+ nonnegative rational weight, whose weights sum to one. The state records
17
+ the data needed to continue a construction; a feature vector records the
18
+ statistics whose expectations must be retained.
19
+
20
+ The next lemma is the constructive finite-dimensional Carath\'eodory
21
+ argument for preserving an expectation. Its connection with moment
22
+ matching is classical~\cite{BayerTeichmann2005}; we include the exact
23
+ elimination and its bit bound because both are needed by the algorithm.
24
+
25
+ \begin{lemma}[Affine support reduction]
26
+ \label{lem:affine-support}
27
+ Let a distribution list have states \(s_1,\ldots,s_M\), weights
28
+ \(\lambda_1,\ldots,\lambda_M\), and feature vectors
29
+ \(v(s_i)\in\mathbb Q^d\). There is an exact algorithm that replaces the
30
+ weights by nonnegative rational weights supported on at most \(d+1\) of
31
+ the same states, preserving
32
+ \[
33
+ \sum_{i=1}^M\lambda_i v(s_i).
34
+ \]
35
+ Its running time and output encoding length are polynomial in the
36
+ encoding length of the given list and feature vectors.
37
+ \end{lemma}
38
+
39
+ \begin{proof}
40
+ Discard zero-weight entries. If more than \(d+1\) remain, choose a
41
+ nonzero integral affine dependence \(z\) satisfying
42
+ \[
43
+ \sum_i z_i=0,
44
+ \qquad
45
+ \sum_i z_i v(s_i)=0.
46
+ \]
47
+ Since its coefficients sum to zero, there are both positive and negative
48
+ coefficients. Set
49
+ \[
50
+ t=\min_{i:z_i>0}\frac{\lambda_i}{z_i},
51
+ \qquad
52
+ \lambda'_i=\lambda_i-tz_i.
53
+ \]
54
+ The new weights are nonnegative, have the same sum and feature
55
+ expectations, and include at least one additional zero. Repeating gives
56
+ the support bound.
57
+
58
+ For completeness, the rational arithmetic has polynomial complexity.
59
+ An affine dependence can be found using at most \(d+2\) columns of the
60
+ matrix with columns \((1,v(s_i))\). Clearing denominators and using
61
+ minors gives an integral dependence of polynomial bit length. If
62
+ \(\lambda_i=b_i/D\) for a common denominator \(D\), and \(j\) attains
63
+ the minimum defining \(t\), then
64
+ \begin{equation}
65
+ \lambda'_i=
66
+ \frac{b_i z_j-b_jz_i}{Dz_j}.
67
+ \label{eq:compression-denominator}
68
+ \end{equation}
69
+ Thus one elimination adds at most the bit length of \(|z_j|\) to a
70
+ common denominator. There are at most \(M\) eliminations, and the
71
+ feature vectors do not change. The resulting bit lengths and the exact
72
+ linear-algebra computations are polynomially bounded.
73
+ \end{proof}
74
+
75
+ Support reduction preserves every property satisfied by each state in
76
+ the list, whether or not that property appears among the features. It
77
+ does not preserve the entire joint distribution or arbitrary future
78
+ adaptive behavior. We therefore specify the retained features at each
79
+ use and verify the required estimates for the resulting process.
80
+
81
+ \subsection{A distribution list for the preparation stage}
82
+
83
+ Let \(M_\star\) denote the number of stars in the preparation
84
+ construction, and write \(X_e\) for the current count of star \(e\).
85
+ Each count remains within its original floor and ceiling. A weighted
86
+ pair update within a strict sign preserves the weighted sum and has
87
+ conditional mean equal to the current count vector. For every pair of
88
+ distinct coordinates \(e,f\), it also satisfies
89
+ \begin{equation}
90
+ \E[X'_e\mid X]=X_e,
91
+ \qquad
92
+ \E[X'_eX'_f\mid X]\le X_eX_f.
93
+ \label{eq:star-local-moments}
94
+ \end{equation}
95
+ Indeed, unless both coordinates are the selected pair, the product is
96
+ affine in the update parameter. If they are the selected pair, their
97
+ increments have opposite signs and the product is concave. A
98
+ one-coordinate rounding with the correct mean preserves every distinct
99
+ pair-product expectation.
100
+
101
+ These assertions hold for every admissible state and every permissible
102
+ choice of the next pair. Thus the next pair may be selected adaptively,
103
+ for example as the first two fractional coordinates in a fixed order.
104
+ After branching one update at every state, apply
105
+ Lemma~\ref{lem:affine-support} with the features
106
+ \[
107
+ X_e \quad\text{and}\quad X_eX_f \qquad(e<f).
108
+ \]
109
+ Induction using~\eqref{eq:star-local-moments} preserves the initial
110
+ first moments and the upper bounds on distinct pair moments. Full
111
+ independence between the positive, negative, and zero-coefficient
112
+ classes is unnecessary for these conclusions.
113
+
114
+ The weighted sums and floor/ceiling restrictions are properties of each
115
+ retained state. Each productive pair update makes at least one
116
+ fractional count integral, and integral counts are never updated again.
117
+ There are therefore only \(O(M_\star)\) updates, with identity updates
118
+ padding states that finish earlier. Ordinary one-coordinate rounding
119
+ also handles the zero coefficients and the final positive-side
120
+ fraction. We leave the final negative-side fraction unrounded until
121
+ these operations are complete. Each compressed list has
122
+ \(O(M_\star^2)\) entries.
123
+
124
+ \paragraph{The final negative-side fraction.}
125
+ Condition on a state of this last list. There is at most one fractional
126
+ count, say \(X_e=m+\xi\), where \(0<\xi<1\). The identity of \(e\)
127
+ may depend on the state. Perform the special rounding of the
128
+ preparation construction: use a nominal coin of mean \(\xi\), open the
129
+ outside supplier according to \(m+1\) if its flag is one, and activate
130
+ the extra deficit on a subset of \(D_e\) with marginal \(\xi\) at
131
+ every target.
132
+
133
+ There is a polynomial-support law for this subset. If
134
+ \(d_e=|D_e|\), choose a size
135
+ \[
136
+ L\in\{\lfloor\xi d_e\rfloor,\lceil\xi d_e\rceil\},
137
+ \qquad \E L=\xi d_e,
138
+ \]
139
+ then choose a uniformly random cyclic interval of length \(L\) in a
140
+ fixed cyclic order of the targets. Each target has inclusion
141
+ probability \(\E L/d_e=\xi\), and the support has size at most
142
+ \(2d_e\). Including the nominal coin changes this bound by only a
143
+ constant factor.
144
+
145
+ For a fixed target, the special star's activation count has conditional
146
+ mean \(X_e\); its nominal count has the same conditional mean. Every
147
+ other star count is integral in the conditioned state. Consequently,
148
+ for any two distinct stars activating this target, the conditional
149
+ expectation of their activation product is the product of their
150
+ current counts. This argument applies separately in every state, so
151
+ it remains valid when the identity of the final fractional star varies.
152
+ After averaging, the activation counts retain the nonpositive
153
+ pair-covariance bounds. Each individual activation count remains
154
+ between the original adjacent integers, giving its variance bound as
155
+ well. No pairwise independence between different targets of this last
156
+ star is required: the deficit estimates are made for one target at a
157
+ time, and the clipping bound sums expectations over targets.
158
+
159
+ \paragraph{Conditional rounding inside bundles.}
160
+ For each resulting outer state, clip the deficits and rescale the
161
+ bundle masses exactly as in Theorem~\ref{thm:preparation}. Keep this
162
+ outer state fixed while constructing a new list for all the
163
+ within-bundle rounds. Successive pair updates and compression of all
164
+ first and distinct-pair moments of the opening vector preserve its
165
+ marginals and nonpositive covariances conditional on this outer
166
+ state. Updates in different bundles preserve cross-bundle product
167
+ expectations; thus their entire Cartesian product need not be
168
+ enumerated.
169
+
170
+ In particular, if \(\eta_i\) is the rounded opening minus its
171
+ conditional mean in the fixed outer state, then the noise on a
172
+ client's old assignment obeys
173
+ \[
174
+ \Var\left(
175
+ \sum_{i\in F_j\cap\bigcup_sP_s}\eta_i
176
+ \,\middle|\,\text{outer state}
177
+ \right)
178
+ \le
179
+ g\sum_s\sum_{i\in F_j\cap P_s}\frac{p'_s}{p_s}y_i
180
+ \le g/p_0\le 2g.
181
+ \]
182
+ Here \(p'_s\le1\) and \(p_s\ge p_0\ge1/2\). This is the conditional
183
+ noise estimate used in the preparation proof. Maintaining a separate
184
+ inner list for every outer state retains this estimate despite
185
+ the varying rescalings.
186
+
187
+ All remaining preparation estimates use the retained first and second
188
+ moments, or properties holding in every state. In particular, supplier
189
+ availability and the raw opening-count bound hold in each state;
190
+ the clipping estimate and the probability of exceeding its count
191
+ allowance follow from the same deficit moments. The preparation list
192
+ therefore satisfies the same unconditioned cost and budget-success
193
+ bounds as the randomized construction. Discarding budget failures
194
+ and selecting a remaining grid solution of minimum total nearest-unit
195
+ assignment cost gives the corresponding deterministic bound on the
196
+ sum over clients. This single choice need not simultaneously attain
197
+ each client's individual expectation bound.
198
+
199
+ \subsection{A distribution list for each physical round}
200
+
201
+ Fix a physical state and a round. For each target copy, first construct
202
+ a small list of source sets of cardinality \(\Delta\) with the
203
+ prescribed edge marginals. Use ordinary fixed-sum pair rounding:
204
+ after each pair update, branch each current state to its at most two
205
+ endpoints and immediately compress the resulting list while preserving
206
+ first moments. Thus no full tree of a target's pair updates is ever
207
+ enumerated, and every intermediate list has polynomial support.
208
+ All sets in this list
209
+ contain the target's own group and respect the edges whose prescribed
210
+ marginal is zero or one.
211
+
212
+ Combine the target lists by successive independent products. After
213
+ each product, compress while retaining every edge first moment and
214
+ every product of two edge indicators belonging to distinct targets.
215
+ On adjoining a new target independently, its edge products with earlier
216
+ targets have the required expectations; compression then preserves
217
+ them. Induction gives a graph list with all the first and cross-target
218
+ second moments of the independent-target graph construction. Its
219
+ feature dimension and support size are polynomial in the number of
220
+ active copies.
221
+
222
+ The ideal generator in~\eqref{eq:rnd-ideal-generator} is linear in
223
+ edge indicators except for the terms \(\delta_hY_h\). Expanding these
224
+ terms gives products of edges from a common source to distinct targets,
225
+ and diagonal terms reducible to first moments. The retained statistics
226
+ therefore suffice for its graph average. The heavy-source rule and
227
+ forced openings depend on more than these moments, but this introduces
228
+ no extra averaging requirement: the batch drift
229
+ bound~\eqref{eq:rnd-batch-drift} holds conditional on every realized
230
+ graph, with that graph's own forced openings and chunks. Only after
231
+ that bound is applied do we average the ideal generator, obtaining
232
+ \eqref{eq:rnd-average-drift} for the compressed graph distribution.
233
+
234
+ \paragraph{Proposal and trigger lists.}
235
+ For every graph, include both round types, each with probability
236
+ \(1/2\). Within either type, construct the proposal or trigger
237
+ indicators by successive independent Bernoulli products, compressing
238
+ after each product while retaining all squarefree monomials of degree
239
+ at most four. These moments coincide exactly with those of the
240
+ independent reference law. There are polynomially many such
241
+ monomials. In the balanced type the variables being compressed are
242
+ the proposals, before conflict filtering.
243
+
244
+ To see why filtering requires no higher moments, write \(Q_h\) for a
245
+ balanced proposal and \(I_h\) for its acceptance. If \(C_h\) is the
246
+ set of sources conflicting with \(h\), then, in every outcome,
247
+ \[
248
+ Q_h-\sum_{t\in C_h}Q_hQ_t\le I_h\le Q_h,
249
+ \qquad
250
+ I_hI_t\le Q_hQ_t\quad(h\ne t).
251
+ \]
252
+ A balanced source has \(|E_h|=\Delta\), and each target has
253
+ \(\Delta\) possible sources, so \(|C_h|\le\Delta(\Delta-1)\).
254
+ Preservation of first and second proposal moments gives
255
+ \begin{equation}
256
+ p_*-\Delta(\Delta-1)p_*^2\le\E I_h\le p_*,
257
+ \qquad
258
+ \E[I_hI_t]\le p_*^2\quad(h\ne t).
259
+ \label{eq:list-conflict-moments}
260
+ \end{equation}
261
+ These are the marginal and pair bounds needed for the isolated-action
262
+ and simultaneous-action estimates. Accepted out-sets remain disjoint
263
+ in every outcome.
264
+
265
+ For an unbalanced round, the count statistic from
266
+ Equation~\eqref{eq:rnd-count-statistic}, conditional on the graph,
267
+ has the form
268
+ \[
269
+ Z_*=
270
+ \sum_e c_e I_e+\sum_{e<f}c_{ef}I_eI_f
271
+ \]
272
+ with fixed rational coefficients. It has degree at most two in the
273
+ trigger indicators, and its square has degree at most four after using
274
+ \(I_e^2=I_e\). The compressed law therefore has exactly the same
275
+ \(\E Z_*\), \(\E Z_*^2\), and \(\Var Z_*\) as the independent
276
+ reference law. The variance estimate proved for independent
277
+ indicators transfers to this law, and hence so does the Chebyshev
278
+ count-failure bound. An independent-coordinate variance inequality
279
+ is applied to the reference law before this transfer.
280
+
281
+ The terminal alive-mass estimate likewise uses only the marginal and
282
+ pair bounds for the \(\Delta\) possible incoming triggers at each
283
+ surviving target. It follows by the same union lower bound as in the
284
+ randomized analysis. Thus all probabilistic estimates in
285
+ Theorem~\ref{thm:grid-rounding} remain valid for these lists.
286
+
287
+ \paragraph{Retaining adaptive histories.}
288
+ Expand these graph and proposal lists at every reached physical
289
+ history, and retain all resulting physical outcomes over the
290
+ \(T\) rounds. The history tree is not compressed. The alive sets
291
+ used in the analysis can be defined along this tree, but need not be
292
+ computed by the algorithm. Even when two histories reach the same
293
+ physical state with different analysis-only alive sets, the
294
+ next-round estimates apply to either history, since they hold for
295
+ every admissible alive set conditional on the current physical state
296
+ and graph.
297
+
298
+ The number of active copies is polynomial: there are at most
299
+ \(\Delta\) at each facility, and resetting regenerates copies at an
300
+ existing facility. The number of chunk actions is also polynomial,
301
+ since the total number of source--target incidences is
302
+ \(\Delta\) times the number of target copies. Each history has only
303
+ polynomially many children. Since \(T\) is an input-independent
304
+ constant, the complete history tree has polynomial size. At each
305
+ leaf perform the final deterministic completion, discard outcomes
306
+ exceeding the additive budget, and select one of minimum total
307
+ connection cost.
308
+
309
+ \subsection{Rational implementation and bit complexity}
310
+
311
+ We give the encoding details because support size alone does not imply
312
+ a polynomial-time algorithm. Fix rational values of all algorithmic
313
+ parameters. In each of the finitely many rounds, fix in advance a
314
+ rational taper value \(\widehat P\) satisfying its stipulated
315
+ accuracy. The analytic functions of elapsed time, the potential, and
316
+ the analysis-only alive-set decisions need not be evaluated by
317
+ the algorithm.
318
+
319
+ An optimal basic LP solution has polynomial encoding length. Splitting
320
+ facilities to make assignments use whole pieces introduces only
321
+ polynomially many pieces. Piece masses, bundle masses, and
322
+ intersection masses are sums and differences of the LP coordinates.
323
+ The extra star weights multiply a deficit by the fixed rational
324
+ \(\gamma\), and conversion to grid counts multiplies by the integer
325
+ \(\Delta\). Hence the initial star counts have a common denominator
326
+ \(D_0\) of polynomial bit length.
327
+
328
+ For weighted pair rounding, write \(a_e=|u_e|\). If a pair update
329
+ makes \(X_e\) integral and leaves \(X_f\) fractional, preservation
330
+ of its weighted sum gives
331
+ \[
332
+ a_fX'_f=a_fX_f+a_eX_e-a_eX'_e.
333
+ \]
334
+ Throughout these updates, therefore, every weighted count lies in
335
+ \(D_0^{-1}\mathbb Z\). Recovering \(X_f\) only divides by the
336
+ polynomially bounded integer \(a_f\). Counts remain in their original
337
+ integer bounds, so their numerators and their endpoint probabilities
338
+ have polynomial bit length as well. Final single-coordinate rounding
339
+ makes the coordinate integral; zero-coefficient counts retain their
340
+ initial values until rounded directly. Clipping and rescaling give
341
+ fresh rational inputs of polynomial bit length for the within-bundle
342
+ rounds, where the same argument applies with unit coefficients.
343
+
344
+ The taper radii can also be computed exactly. On an interval where
345
+ \(m\) source copies have saturated marginal one and \(r\) source
346
+ copies have marginal strictly between zero and one, the radius
347
+ equation is
348
+ \[
349
+ m+\frac{r}{\widehat P}
350
+ -\frac{\sum_{h\text{ partial}}d(i,h)}{\widehat P N_i}
351
+ =\Delta.
352
+ \]
353
+ When \(r>0\), an interior solution is
354
+ \begin{equation}
355
+ N_i=
356
+ \frac{\sum_{h\text{ partial}}d(i,h)}
357
+ {r+\widehat P(m-\Delta)}.
358
+ \label{eq:rational-taper-radius}
359
+ \end{equation}
360
+ The breakpoints are the rational numbers \(d(i,h)\) and
361
+ \(d(i,h)/(1-\widehat P)\). Sorting these values and checking the
362
+ successive intervals finds the smallest solution, including a
363
+ breakpoint solution. If \(r=0\), the equation is constant on the
364
+ interval, and the first point of a solution interval is a breakpoint.
365
+ The separately prescribed case of sufficient
366
+ co-located mass uses \(N_i=0\). All radii, marginals, and resulting
367
+ branch probabilities have polynomial bit length. The physical states
368
+ and their feature values are determined without reference to the
369
+ list weights.
370
+
371
+ It remains to control the list weights across repeated branching and
372
+ compression. Suppose a feature vector has \(d\) coordinates of bit
373
+ length at most \(L\). In the affine-dependence computation, clearing
374
+ denominators in each row of the matrix on at most \(d+2\) columns
375
+ produces integer entries of bit length \(O(dL)\). A nonzero kernel
376
+ vector can be chosen using minors, with bit length
377
+ \(O(d^2L+d\log(d+1))\) by the determinant bound. These bounds are
378
+ independent of the current list weights.
379
+
380
+ By~\eqref{eq:compression-denominator}, an elimination multiplies a
381
+ common weight denominator by just one coefficient of such a
382
+ dependence. An exact branch with probability denominator \(q\)
383
+ multiplies a common denominator by at most \(q\). Branching a whole
384
+ list adds the bit lengths of only polynomially many such
385
+ denominators, and taking a product of lists adds their denominator
386
+ bit lengths. There are polynomially many list operations, including
387
+ the entire constant-depth physical history tree. Their common
388
+ denominators and numerators consequently retain polynomial bit
389
+ lengths. Exact linear algebra, comparisons, and cost evaluations
390
+ therefore give a deterministic algorithm whose bit complexity is
391
+ polynomial in the input encoding length for every fixed choice of
392
+ accuracy parameters.
393
+
394
+ \subsection{Loss allocation and the approximation theorem}
395
+
396
+ We first record explicitly how conditioning and deterministic
397
+ selection are combined. For a nonnegative cost \(C\) and an event
398
+ \(G\) with \(\Prob(G)\ge1-r\),
399
+ \begin{equation}
400
+ \E[C\mid G]
401
+ \le\frac{\E C}{1-r}.
402
+ \label{eq:conditioning-cost}
403
+ \end{equation}
404
+ Thus a finite distribution list contains a successful outcome whose
405
+ cost is no more than the right-hand side. No independence between
406
+ cost and budget success is required.
407
+
408
+ \begin{theorem}[Deterministic additive approximation]
409
+ \label{thm:pseudo}
410
+ For every fixed \(\varepsilon>0\), there is an
411
+ instance-independent integer \(c\ge0\) and a deterministic
412
+ polynomial-time algorithm for metric \(k\)-median that opens at
413
+ most \(k+c\) facilities and has total connection cost at most
414
+ \[
415
+ \left(1+\frac2e+\varepsilon\right)\operatorname{LP},
416
+ \]
417
+ where \(\operatorname{LP}\) is the optimum value of the assignment
418
+ relaxation. In particular, its cost is at most the same factor times
419
+ \(\OPT_k\).
420
+ \end{theorem}
421
+
422
+ \begin{proof}
423
+ Put \(\alpha_\star=1+2/e\), and choose a fixed positive rational
424
+ number
425
+ \[
426
+ t\le\min\{1/8,\varepsilon/10\}.
427
+ \]
428
+ Choose the parameters in the constructions underlying
429
+ Theorems~\ref{thm:preparation} and~\ref{thm:grid-rounding} with
430
+ unconditioned cost factors at most \(1+t\) and
431
+ \(\alpha_\star+t\), respectively, and with their respective
432
+ budget-failure probabilities at most \(t\). The proofs of those
433
+ theorems allow the cost and failure tolerances to be made
434
+ arbitrarily small; their stated expectation guarantees absorb this
435
+ same conditioning loss. Here we keep the loss visible.
436
+
437
+ All parameter choices can be made in a consistent order. After the
438
+ preparation parameters other than the grid are fixed, take an even
439
+ integer \(\Delta\) sufficiently large, set \(g=1/\Delta\), and
440
+ take a rational horizon of order
441
+ \(1+\log(\Delta/t)\). The requirements that the terminal error
442
+ be small and that \(\Lambda g\) be small are compatible because
443
+ \(\log\Delta/\Delta\to0\). Then choose the taper tolerance,
444
+ the selection bias, and the time step successively small. The
445
+ number of rounds is now fixed. Finally choose the heavy-source
446
+ parameter sufficiently small that the sum of the conditional
447
+ count-failure probabilities over all rounds is at most \(t\).
448
+ The resulting additive opening allowances are constants depending
449
+ only on these parameter choices.
450
+
451
+ Let \(L=\operatorname{LP}\). Apply the preparation list to an
452
+ optimal LP solution. Its total nearest-unit cost has expectation at
453
+ most \((1+t)L\), and its budget event has probability at least
454
+ \(1-t\). Select the least expensive successful grid solution.
455
+ By~\eqref{eq:conditioning-cost}, its total nearest-unit cost
456
+ \(L_{\rm grid}\) satisfies
457
+ \[
458
+ L_{\rm grid}\le\frac{1+t}{1-t}L.
459
+ \]
460
+ Apply the physical-rounding list to this fixed grid solution. The
461
+ summed cost bound is at most \((\alpha_\star+t)L_{\rm grid}\)
462
+ before discarding count failures, and the budget succeeds with
463
+ probability at least \(1-t\). Selecting the least expensive
464
+ successful integral output therefore gives cost at most
465
+ \[
466
+ \frac{(1+t)(\alpha_\star+t)}{(1-t)^2}L.
467
+ \]
468
+ Since \(\alpha_\star<2\) and \(t\le1/8\),
469
+ \begin{align*}
470
+ \frac{(1+t)(\alpha_\star+t)}{(1-t)^2}-\alpha_\star
471
+ &=
472
+ \frac{(3\alpha_\star+1)t+(1-\alpha_\star)t^2}
473
+ {(1-t)^2}\\
474
+ &\le\frac{7t}{(1-t)^2}
475
+ <10t
476
+ \le\varepsilon.
477
+ \end{align*}
478
+ The two additive allowances sum to an instance-independent
479
+ constant, which may be rounded up to an integer \(c\).
480
+
481
+ Both minimum-cost selections are computable on polynomial-size
482
+ lists, with polynomial bit complexity as proved above. They use
483
+ total costs; the deterministic grid solution is not required to
484
+ attain every client's individual expectation bound. If \(L=0\),
485
+ the nonnegative cost has expectation zero in the preparation list
486
+ and then in the physical-rounding list, so the same argument gives
487
+ zero cost without division by \(L\).
488
+
489
+ Every opened copy lies at an original candidate facility. Merge
490
+ copies introduced by the construction back to their original
491
+ facility. This preserves connection distances and cannot increase
492
+ the number of opened facilities. Finally,
493
+ \(\operatorname{LP}\le\OPT_k\), proving the last assertion.
494
+ \end{proof}
495
+
496
+ \subsection{Applying the reduction on rational inputs}
497
+ \label{sec:reduction-implementation}
498
+
499
+ Before applying Theorem~\ref{thm:li-svensson}, we record its interface
500
+ with the deterministic algorithm just proved. Every call of that reduction
501
+ uses the same clients and distances with a restricted candidate set
502
+ \(F'\subseteq F\); our pseudo-algorithm uses no additional input promise
503
+ or prescribed-open facilities. Its internal forced openings are decisions
504
+ of that call, not constraints passed from another call. Copies are merged
505
+ back to original candidates before returning its output. If
506
+ \(0<|F'|<k\), opening every candidate gives the optimum for that restricted
507
+ instance. If \(F'=\varnothing\) and clients remain, discard the branch.
508
+ The distinguished branch retaining a padded optimal \(k\)-set has
509
+ neither exception. When the additive allowance is zero, the
510
+ pseudo-algorithm already satisfies the required budget.
511
+
512
+ The zero-optimum case can be recognized before the reduction. Every
513
+ client location must be an available candidate location, and there can
514
+ be at most \(k\) distinct client locations. Equivalently, every
515
+ zero-distance class containing a client must contain a candidate, and
516
+ there are at most \(k\) such client classes. These conditions are necessary
517
+ and sufficient in the original metric; when they hold, open those
518
+ locations. Thus the positive-optimum analysis of the reduction does not
519
+ require division by zero. Co-located pieces occur only inside our
520
+ pseudo-algorithm and do not change this original-metric test.
521
+
522
+ We also make explicit a rational implementation of the deletion threshold
523
+ in the proof of Li--Svensson's reduction~\cite[Section~2, Algorithm~2]{LiSvensson2016}.
524
+ That proof analyzes a threshold determined by the unknown optimum.
525
+ Its numerical value need not be computed. Suppose a call returns a set
526
+ \(T\) with \(k<|T|\le k+c\). For every set \(T'\subseteq T\) obtainable
527
+ by at most \(c\) deletions with \(|T'|>k\), and every \(i\in T'\), compute
528
+ \[
529
+ \Delta(T',i)=\cost(T'\setminus\{i\})-\cost(T').
530
+ \]
531
+ These numbers are nonnegative rationals of polynomial bit length.
532
+ There are \(n^{O(c)}\) such numbers. Run the reduction's deletion phase
533
+ for each distinct number as threshold, and for zero, with a fixed order
534
+ for choosing deletions; follow each run by its prescribed enumerative
535
+ completion and retain the cheapest feasible result.
536
+
537
+ To justify this replacement, let \(B^*\ge0\) be the threshold used in
538
+ the reduction's analysis. Choose the largest enumerated value at most
539
+ \(B^*\), including equality, or zero if there is none. Every test of the form
540
+ \(\Delta(T',i)\le B^*\) has the same answer at this representative
541
+ threshold. Induction through the at most \(c\) deletions therefore
542
+ reproduces the ideal deletion history, including its fixed tie choices.
543
+ Its output is present among the enumerated outputs. The approximation
544
+ analysis still uses \(B^*\); the algorithm uses only exact rational
545
+ comparisons. This adds \(n^{O(c)}\) overhead to the stated reduction.
546
+ All candidate enumeration, distance comparisons and cost evaluations
547
+ likewise use polynomial-bit rational arithmetic.
548
+
549
+ Finally, the approximation parameter supplied to the reduction can be a
550
+ fixed rational upper bound on our ratio, with its excess charged to the
551
+ allowed accuracy. The auxiliary positive constants in its proof may then
552
+ be chosen rational as well. These observations preserve both determinism
553
+ and polynomial binary-input time; they require no oracle for the optimum.
554
+
555
+ \begin{proof}[Proof of Theorem~\ref{thm:main}]
556
+ Fix \(\varepsilon>0\). Apply Theorem~\ref{thm:pseudo} with
557
+ loss \(\varepsilon/4\), obtaining a deterministic
558
+ \(c\)-additive approximation, where \(c\) depends only on this fixed
559
+ loss. Choose a fixed rational number \(\alpha\) with
560
+ \[
561
+ 1+2/e+\varepsilon/4<\alpha<1+2/e+\varepsilon/2.
562
+ \]
563
+ The pseudo-algorithm is a \(c\)-additive \(\alpha\)-approximation.
564
+ The additive-to-ordinary reduction of Theorem~\ref{thm:li-svensson},
565
+ with a fixed positive rational loss at most \(\varepsilon/2\) and the
566
+ implementation in Section~\ref{sec:reduction-implementation},
567
+ gives a deterministic polynomial-time
568
+ algorithm opening at most \(k\) original facilities and having
569
+ cost at most
570
+ \[
571
+ \left(1+\frac2e+\varepsilon\right)\OPT_k.
572
+ \]
573
+ Copies can be merged back to their original facilities as above.
574
+ If exactly \(k\) facilities are required, add unused facilities
575
+ from \(F\), which is possible because \(k\le|F|\) and can only
576
+ decrease the cost.
577
+
578
+ \end{proof}
579
+
580
+ Combining Theorem~\ref{thm:main} with the hardness bound recalled in
581
+ Section~\ref{sec:introduction} proves Corollary~\ref{cor:threshold}:
582
+ under \(P\ne NP\), the infimum of deterministic polynomial-time
583
+ approximation factors in the specified candidate-facility model is
584
+ \(1+2/e\). The upper bound holds for every fixed positive loss and
585
+ does not require attainment of the endpoint.
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/inequality.tex ADDED
@@ -0,0 +1,365 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A finite inequality for the drift}
2
+ \label{sec:inequality}
3
+
4
+ The cost analysis uses an inequality on a finite probability space. Its
5
+ comparison matrix need not be symmetric. The proof allows a positive
6
+ contribution at one index only by charging indices with smaller values;
7
+ the negative contributions at those indices pay the entire charge.
8
+
9
+ The statement below is independent of the rounding construction.
10
+ Section~\ref{sec:rounding} will apply it to normalized client distances
11
+ and directed edge probabilities; Equation~\ref{eq:rnd-normalization}
12
+ records that substitution. We prove the finite statement first so that
13
+ the geometric analysis can use it as a single input.
14
+
15
+ For $0\le x\le1$, define
16
+ \begin{equation}
17
+ \label{eq:analytic-coefficients}
18
+ \begin{aligned}
19
+ A(x)&=1+2\int_0^1(1-e^{-tx})\,dt,&
20
+ P(x)&=\int_0^1te^{-tx}\,dt,\\
21
+ B(x)&=2P(x),& m(x)&=A(x)-1-2xP(x).
22
+ \end{aligned}
23
+ \end{equation}
24
+ We suppress the argument $x$ when it is fixed. Differentiation under the
25
+ integral gives $A'=B$ and
26
+ $A''(x)=-2\int_0^1t^2e^{-tx}\,dt<0$. In particular,
27
+ $0<P\le1/2$ and $m\ge0$, the latter by concavity and $A(0)=1$.
28
+ Integration by parts also gives
29
+ \begin{equation}
30
+ \label{eq:analytic-identities}
31
+ (1+x)(A-1)=2x(1-P),\qquad
32
+ (1+x)A+xB-1=3x,\qquad A(1)=1+\frac2e.
33
+ \end{equation}
34
+ These identities hold at $x=0$ as well, using the integral definitions.
35
+
36
+ \begin{theorem}[Finite comparison inequality]
37
+ \label{thm:finite-inequality}
38
+ Let $I$ be a finite index set with probability weights $(\pi_i)_{i\in I}$,
39
+ and let $D_i\ge0$ satisfy $\E_iD_i=1$. Both $\E_i$ and $\E_t$ denote
40
+ expectation with these weights; in a double expectation the two indices
41
+ are sampled independently. Fix $0\le x\le1$ and $0<y\le1$, and set
42
+ \[
43
+ \Theta=\frac{P(y-x)^2}{y}.
44
+ \]
45
+ Suppose $q_{ti}\in[0,1]$ and $R_i\ge0$ satisfy
46
+ \begin{equation}
47
+ \label{eq:finite-comparison}
48
+ R_i(1-Pq_{ti})\le D_i+D_t\qquad\text{whenever }q_{ti}<1.
49
+ \end{equation}
50
+ No symmetry is assumed for $q$. For any $s_i\in[0,1]$, put
51
+ $r_i=\E_tq_{ti}$ and $C_i=1-Ps_i$. Then
52
+ \begin{equation}
53
+ \label{eq:finite-inequality}
54
+ \begin{aligned}
55
+ \E_i\Big[&C_i(1-r_i)R_i
56
+ +r_i\{mD_i+(2-s_i)Py(D_i+1)\}-C_i(D_i+1)\\
57
+ &\hspace{12mm}
58
+ -\E_t(1-q_{ti})\bigl(D_t-(1+m+2Py)D_i\bigr)_+\Big]
59
+ \le2\Theta.
60
+ \end{aligned}
61
+ \end{equation}
62
+ Here $u_+=\max(u,0)$.
63
+ \end{theorem}
64
+
65
+ The proof will bound each positive row by charges sent to indices with
66
+ smaller $D$ values, then show that those receiving rows pay all incoming
67
+ charges. The scalar estimates below locate the positive rows, bound the
68
+ largest value they can charge, and certify the required negative
69
+ contributions. Every terminating decimal denotes an exact rational number.
70
+
71
+ \begin{lemma}[Scalar bounds]
72
+ \label{lem:scalar-bounds}
73
+ Fix $x\in[0,1]$, put $X=1-x$, and take
74
+ $0\le w\le X$ and $s\in\{0,1\}$. Use the functions in
75
+ Equation~\eqref{eq:analytic-coefficients}, and define
76
+ \begin{equation}
77
+ \label{eq:scalar-parameters}
78
+ \begin{aligned}
79
+ z&=Pw^2,& b&=(2-s)P(x+w),& a&=A+2Pw,& C&=1-Ps,\\
80
+ d_0&=.52,& d_1&=.4,& H_0&=.394-.42X^2+.04X^3,& H_1&=.25,\\
81
+ J_s&=CH_s,&
82
+ k_s&=(1-s)\frac{1-\sqrt{1-P}}{1+\sqrt{1-P}}.
83
+ \end{aligned}
84
+ \end{equation}
85
+ For $q,r\in[0,1]$, set
86
+ \begin{equation}
87
+ \label{eq:scalar-functions}
88
+ \begin{aligned}
89
+ \psi(q)&=\frac{1-q}{1-Pq},&
90
+ \kappa_s(q)&=C\psi(q)-(1-q),\\
91
+ K(r)&=C-k_s-br+1.6z,&
92
+ L(r)&=(C-m-b)r+.4z,\\
93
+ M(r)&=(1-r)a+CPr,& G(r)&=M(r)-L(r).
94
+ \end{aligned}
95
+ \end{equation}
96
+ Then the following five bounds hold on the indicated domains:
97
+ \begin{align}
98
+ m+b-\frac{.4z}{r}
99
+ &\le\frac{C(1-P)}{1-Pr}
100
+ &&(0<r\le1),
101
+ \label{eq:scalar-first}\\
102
+ L(r)\ge0,\qquad K(r)>0,\qquad K(r)
103
+ &\ge d_sG(r)
104
+ &&(0\le r\le1),
105
+ \label{eq:scalar-linear}\\
106
+ \bigl((J_s-b)r+1.6z\bigr)M(r)
107
+ +(C-k_s-J_sr)L(r)
108
+ &\ge0
109
+ &&(0\le r\le1),
110
+ \label{eq:scalar-charge}\\
111
+ C-k_s+1.6z-bq+.52\bigl(k_s-\kappa_s(q)\bigr)
112
+ &\ge H_0
113
+ &&(0\le q\le1),
114
+ \label{eq:scalar-type-zero}\\
115
+ C-k_s+1.6z-b&\ge.25.
116
+ \label{eq:scalar-type-one}
117
+ \end{align}
118
+ \end{lemma}
119
+
120
+ \begin{proof}
121
+ The scalar bounds are proved in Appendix~\ref{app:certificates} by
122
+ analytic reductions and exact polynomial certificates.
123
+ \end{proof}
124
+
125
+ \begin{proof}[Proof of Theorem~\ref{thm:finite-inequality}]
126
+ We may discard indices of probability zero. The proof treats the
127
+ quantities with a fixed second index $i$ as a row, with $t$ indexing its
128
+ columns.
129
+
130
+ \paragraph{Reduction of the parameters.}
131
+ For fixed $x,D,q,R,s$, the left side of
132
+ Equation~\eqref{eq:finite-inequality} is nondecreasing in $y$.
133
+ The coefficient of its linear $y$ term is nonnegative, and increasing
134
+ $y$ decreases the positive part that is subtracted. Replace $y$ there
135
+ by $\max(x,y)=x+w$, where $0\le w\le X=1-x$, and put $z=Pw^2$.
136
+ If $y<x$, then $z=0\le\Theta$; otherwise
137
+ $z=P(y-x)^2\le\Theta$, since $y\le1$. It is therefore sufficient to
138
+ bound the modified left side by $2z$.
139
+
140
+ This modified left side is affine separately in every $s_i$, and its
141
+ hypotheses do not constrain $s_i$. Its maximum over $[0,1]^I$ is
142
+ attained with every $s_i\in\{0,1\}$. Fix such a choice. For each row
143
+ use the notation of Lemma~\ref{lem:scalar-bounds}, with $s=s_i$, and
144
+ temporarily suppress the row subscript. Write $D=D_i$, $R=R_i$,
145
+ $q=q_{ti}$, $Z=D_t$, and $r=\E_tq_{ti}$, and put
146
+ \[
147
+ U=mD+b(D+1).
148
+ \]
149
+ Notice that $a=1+m+2P(x+w)$. Define the row contribution
150
+ \begin{equation}
151
+ \label{eq:row-contribution}
152
+ F=C(1-r)R+Ur-C(D+1)
153
+ -\E_t(1-q)(Z-aD)_+-(.4D+1.6)z.
154
+ \end{equation}
155
+ Because $\E_iD_i=1$, proving $\E_iF_i\le0$ proves the desired
156
+ bound $2z$.
157
+
158
+ \paragraph{A centered majorant for each row.}
159
+ For $s=0$, direct maximization gives
160
+ \[
161
+ \kappa_0(q)=\frac{Pq(1-q)}{1-Pq}
162
+ \le\frac{1-\sqrt{1-P}}{1+\sqrt{1-P}}=k_0.
163
+ \]
164
+ For $s=1$, one has
165
+ $\kappa_1(q)=-P(1-q)^2/(1-Pq)\le0=k_1$.
166
+ Also
167
+ \begin{equation}
168
+ \label{eq:psi-bound}
169
+ \psi(q)=1-q+Pq\psi(q)\le1-q+Pq,
170
+ \end{equation}
171
+ since $\psi(q)\le1$.
172
+
173
+ Equation~\eqref{eq:finite-comparison} implies
174
+ $(1-q)R\le\psi(q)(D+Z)$ when $q<1$. This last inequality also holds
175
+ when $q=1$, as both sides are zero. Using
176
+ $(Z-aD)_+\ge Z-aD$ in Equation~\eqref{eq:row-contribution} gives
177
+ \begin{align*}
178
+ F\le\E_t\big[&Uq+D\{C\psi(q)+a(1-q)-C\}
179
+ -(.4D+1.6)z-C+\kappa_s(q)Z\big].
180
+ \end{align*}
181
+ The centering identity
182
+ \[
183
+ \E_t[\kappa_s(q)Z]
184
+ =k_s-\E_t[(k_s-\kappa_s(q))Z]
185
+ \]
186
+ uses $\E_tZ=1$. Thus, defining the explicit function
187
+ \begin{equation}
188
+ \label{eq:centered-integrand}
189
+ \begin{aligned}
190
+ I_s(D;q,Z)={}&[mD+b(D+1)]q
191
+ +D\{C\psi(q)+a(1-q)-C\}\\
192
+ &-(.4D+1.6)z-C+k_s-(k_s-\kappa_s(q))Z,
193
+ \end{aligned}
194
+ \end{equation}
195
+ we have
196
+ \begin{equation}
197
+ \label{eq:centered-row-bound}
198
+ F_i\le\E_t I_{s_i}(D_i;q_{ti},D_t).
199
+ \end{equation}
200
+ The replacement of $k_sZ$ by $k_s$ is made only under expectation.
201
+ Subsequent pointwise bounds will concern the function in
202
+ Equation~\eqref{eq:centered-integrand}.
203
+
204
+ Since $k_s-\kappa_s(q)\ge0$ and $Z\ge0$, dropping the last term and
205
+ using Equation~\eqref{eq:psi-bound} yields
206
+ \begin{equation}
207
+ \label{eq:pointwise-linear-majorant}
208
+ I_s(D;q,Z)\le DG(q)-K(q).
209
+ \end{equation}
210
+ Both $G$ and $K$ are affine in their argument, so averaging gives
211
+ \begin{equation}
212
+ \label{eq:row-linear-majorant}
213
+ F\le DG(r)-K(r).
214
+ \end{equation}
215
+
216
+ \paragraph{Charges issued by positive rows.}
217
+ If $r=0$, then $q=0$ at every column and averaging
218
+ Equation~\eqref{eq:finite-comparison} gives $R\le D+1$.
219
+ Equation~\eqref{eq:row-contribution} then gives $F\le0$.
220
+ Consequently a row with $F>0$ has $r>0$. By
221
+ Equations~\eqref{eq:scalar-linear} and
222
+ \eqref{eq:row-linear-majorant}, it also has
223
+ \begin{equation}
224
+ \label{eq:positive-row-location}
225
+ G(r)>0,\qquad D>\frac{K(r)}{G(r)}\ge d_s.
226
+ \end{equation}
227
+ In this row put
228
+ \[
229
+ U'=\frac{Ur-(.4D+1.6)z}{Cr}.
230
+ \]
231
+ The identity
232
+ \[
233
+ U'=\frac{D+1}{C}\left(m+b-\frac{.4z}{r}\right)
234
+ -\frac mC-\frac{1.2z}{Cr}
235
+ \]
236
+ and Equation~\eqref{eq:scalar-first} imply
237
+ \begin{equation}
238
+ \label{eq:positive-row-uprime}
239
+ U'\le\frac{(D+1)(1-P)}{1-Pr}.
240
+ \end{equation}
241
+ On the other hand, discarding the nonpositive hinge term in
242
+ Equation~\eqref{eq:row-contribution} gives
243
+ $F/C\le(1-r)R+rU'-(D+1)$.
244
+ If $R\le(D+1)/(1-Pr)$, Equation~\eqref{eq:positive-row-uprime}
245
+ makes this upper bound nonpositive. Therefore
246
+ \begin{equation}
247
+ \label{eq:positive-row-radius}
248
+ R>\frac{D+1}{1-Pr},\qquad U'\le R(1-P).
249
+ \end{equation}
250
+ In particular $r=1$ is impossible for a positive row, since
251
+ Equation~\eqref{eq:positive-row-uprime} would then give $U'\le D+1$.
252
+
253
+ For every column with $q<1$, Equations~\eqref{eq:finite-comparison}
254
+ and \eqref{eq:positive-row-radius} now give
255
+ \[
256
+ (1-q)R+qU'\le R(1-Pq)\le D+Z.
257
+ \]
258
+ For $q=1$, the excess of the left side over $D+Z$ is exactly
259
+ $U'-D-Z$. Using $\E_tZ=1$ and again discarding the nonpositive
260
+ hinge term, we obtain
261
+ \begin{equation}
262
+ \label{eq:positive-row-excess}
263
+ F\le C\E_t\big[\ind_{\{q=1\}}(U'-D-Z)_+\big]
264
+ \le C\E_t(U'-D-Z)_+.
265
+ \end{equation}
266
+ This treats the unconstrained columns with $q=1$ explicitly.
267
+
268
+ It remains to bound the largest value to which this row can charge.
269
+ An exact rearrangement gives
270
+ \[
271
+ U'-D=\frac{br-1.6z-L(r)D}{Cr}.
272
+ \]
273
+ Set $T=(J_s-b)r+1.6z$. The expression in
274
+ Equation~\eqref{eq:scalar-charge} is
275
+ \begin{equation}
276
+ \label{eq:charge-scalar-rearrangement}
277
+ TM(r)+(C-k_s-J_sr)L(r)=TG(r)+K(r)L(r)\ge0.
278
+ \end{equation}
279
+ Using $L(r)\ge0$ and Equation~\eqref{eq:positive-row-location},
280
+ we conclude that
281
+ \[
282
+ br-1.6z-L(r)D
283
+ \le br-1.6z-\frac{L(r)K(r)}{G(r)}\le J_sr.
284
+ \]
285
+ Thus $U'-D\le H_s$. Since $C\le1$,
286
+ Equation~\eqref{eq:positive-row-excess} proves
287
+ \begin{equation}
288
+ \label{eq:outgoing-charge}
289
+ F_i\le\E_t(H_{s_i}-D_t)_+\qquad(F_i>0).
290
+ \end{equation}
291
+ The function $H_0$ decreases from $.394$ to $.014$ on $[0,1]$,
292
+ and $H_1=.25$. Consequently every nonzero charge in
293
+ Equation~\eqref{eq:outgoing-charge} goes to an index with $D_t<.394$.
294
+ This separates every possible receiving index from all positive rows,
295
+ which have $D_i>d_{s_i}\ge.4$. It remains to prove that the negative
296
+ contribution of each receiving row covers the total charge it receives.
297
+
298
+ \paragraph{Negative rows cover the incoming charges.}
299
+ Put $c_*=.394$ and define
300
+ \[
301
+ \mathcal P=\{i:F_i>0\},\qquad
302
+ \mathcal S=\{i:D_i\le c_*\},\qquad
303
+ \Gamma_{it}=\ind_{\{i\in\mathcal P\}}(H_{s_i}-D_t)_+.
304
+ \]
305
+ Equation~\eqref{eq:positive-row-location} shows that
306
+ $\mathcal P\cap\mathcal S=\varnothing$, because $d_s\ge.4>c_*$.
307
+ We claim that every $i\in\mathcal S$ satisfies
308
+ \begin{equation}
309
+ \label{eq:incoming-charge}
310
+ F_i+\E_t\Gamma_{ti}\le0.
311
+ \end{equation}
312
+
313
+ Fix such an $i$ and a column $t$. Hold $q=q_{ti}$, $Z=D_t$,
314
+ the two types $s_i,s_t$, and $\chi=\ind_{\{F_t>0\}}$ fixed.
315
+ As a function of a variable $D\in[0,c_*]$,
316
+ \[
317
+ I_{s_i}(D;q,Z)+\chi(H_{s_t}-D)_+
318
+ \]
319
+ is convex: the first term is affine and the second is a positive part
320
+ multiplied by a nonnegative constant. It suffices to bound this
321
+ expression at $D=0,c_*$. This check concerns the explicit majorant;
322
+ it does not require the comparison hypothesis to remain valid when
323
+ the variable $D$ changes.
324
+
325
+ At $D=c_*$, the incoming charge is zero. By
326
+ Equation~\eqref{eq:pointwise-linear-majorant}, the remaining term is
327
+ at most $c_*G(q)-K(q)\le0$. Indeed, if $G(q)<0$, use $K(q)>0$;
328
+ otherwise use $K(q)\ge d_{s_i}G(q)$ and $c_*<d_{s_i}$.
329
+
330
+ At $D=0$, Equation~\eqref{eq:centered-integrand} reads
331
+ \[
332
+ I_{s_i}(0;q,Z)
333
+ =bq-1.6z-C+k_s-(k_s-\kappa_s(q))Z,
334
+ \]
335
+ where the unindexed scalar parameters belong to row $i$.
336
+ If $\chi=1$ and $s_t=0$, the positive donor row $t$ satisfies
337
+ $Z=D_t>d_0=.52$. Since $k_s-\kappa_s(q)\ge0$,
338
+ Equation~\eqref{eq:scalar-type-zero} gives
339
+ $I_{s_i}(0;q,Z)\le-H_0$, which covers its incoming charge.
340
+ In the other cases the charge is either zero or $H_1=.25$.
341
+ Equation~\eqref{eq:scalar-type-one}, together with $q\le1$,
342
+ gives
343
+ \[
344
+ I_{s_i}(0;q,Z)\le b-1.6z-C+k_s\le-.25,
345
+ \]
346
+ which covers these cases as well. Convexity proves the pointwise
347
+ bound throughout $[0,c_*]$. Apply it at $D=D_i$ and average over
348
+ $t$ in Equation~\eqref{eq:centered-row-bound} to obtain
349
+ Equation~\eqref{eq:incoming-charge}.
350
+
351
+ Finally, the incoming charge is $\Gamma_{ti}$ by definition, and
352
+ exchanging the two finite sums requires no symmetry of $q$.
353
+ Equation~\eqref{eq:outgoing-charge} bounds all
354
+ positive rows by their outgoing charges;
355
+ Equation~\eqref{eq:incoming-charge} makes all receiving rows pay
356
+ their incoming charges; all other rows have nonpositive contribution.
357
+ Every nonzero $\Gamma_{it}$ has $i\in\mathcal P$ and
358
+ $t\in\mathcal S$. Exchanging the two indices in the finite sum with
359
+ weights $\pi_i\pi_t$ therefore gives
360
+ \[
361
+ \E_iF_i\le\E_{i,t}\Gamma_{it}-\E_{i,t}\Gamma_{ti}=0.
362
+ \]
363
+ This proves the stronger bound $2z$ after the parameter reduction and,
364
+ since $z\le\Theta$, proves Equation~\eqref{eq:finite-inequality}.
365
+ \end{proof}
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/introduction.tex ADDED
@@ -0,0 +1,196 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Introduction}\label{sec:introduction}
2
+
3
+ In metric \(k\)-median, a finite set \(J\) of clients and a finite set \(F\)
4
+ of candidate facilities lie in a common metric space. Given an integer \(k\),
5
+ one chooses at most \(k\) facilities to minimize the sum of the distances
6
+ from clients to their nearest chosen facility. For a nonempty set
7
+ \(S\subseteq F\), write
8
+ \[
9
+ d(j,S)=\min_{i\in S}d(j,i),\qquad
10
+ \cost(S)=\sum_{j\in J}d(j,S),\qquad
11
+ \OPT_k=\min_{\substack{S\subseteq F\\1\le|S|\le k}}\cost(S).
12
+ \]
13
+ The input distances are rational and encoded in binary, and
14
+ \(1\le k\le |F|\). Both \(k\) and the metric are unrestricted.
15
+ Candidate facilities are specified as part of the input; we do not
16
+ require \(F=J\). The empty-client instance has cost zero and can be
17
+ handled immediately.
18
+
19
+ The facility budget is a central difficulty: a solution with small
20
+ connection cost can be much easier to obtain when extra facilities are
21
+ allowed. Our approach first permits a constant additive surplus, makes
22
+ that approximation deterministic, and then removes the surplus using an
23
+ established reduction.
24
+
25
+ \begin{theorem}\label{thm:main}
26
+ For every fixed \(\varepsilon>0\), there is a deterministic algorithm which,
27
+ given a finite rational metric \(k\)-median instance with \(1\le k\le |F|\),
28
+ returns \(S\subseteq F\), \(|S|\le k\), such that
29
+ \[
30
+ \sum_{j\in J}d(j,S)\le
31
+ \left(1+\frac2e+\varepsilon\right)\OPT_k.
32
+ \]
33
+ Its running time is polynomial in the binary encoding length of the instance.
34
+ The polynomial may depend on \(\varepsilon\).
35
+ \end{theorem}
36
+
37
+ Hardness below \(1+2/e\) in this facility model follows from the
38
+ Max-\(k\)-Coverage gap: covered clients have distance one and uncovered
39
+ clients have distance at least three. We use the formulation under \(P\ne NP\)
40
+ recorded by Anand and Lee~\cite[Sections~1 and~1.1]{AnandLee2024}, based on
41
+ Feige's perfect-completeness coverage gap~\cite[Theorem~5.3]{Feige1998}.
42
+ For an explicit metric completion, represent sets by facilities and
43
+ universe elements by a disjoint client set. Give distinct points within
44
+ either part distance two, and give a facility--client pair distance one
45
+ for incidence and three otherwise. This is a metric: a same-part edge
46
+ of length two is bounded by \(1+1\), and a cross-part edge of length at
47
+ most three is bounded by \(2+1\). For a universe of size \(m\), the
48
+ connection cost is exactly \(3m-2c\) when the chosen sets cover \(c\)
49
+ elements; a perfect cover has cost \(m\). Thus a gap between
50
+ covering every element and covering at most a
51
+ \(1-1/e+\delta\) fraction gives the lower bound
52
+ \(1+2/e-2\delta\), for every fixed positive \(\delta\).
53
+ Together with Theorem~\ref{thm:main},
54
+ this proves the following consequence.
55
+
56
+ \begin{corollary}\label{cor:threshold}
57
+ If \(P\ne NP\), the infimum of deterministic polynomial-time approximation
58
+ factors for metric \(k\)-median with specified candidate facilities is \(1+2/e\).
59
+ \end{corollary}
60
+
61
+ The infimum in Corollary~\ref{cor:threshold} does not assert attainment of the
62
+ endpoint factor. The hardness assumption and candidate-facility model are part
63
+ of the statement. In particular, the corresponding lower-bound question with
64
+ the restriction \(F=J\) is different~\cite{AnandLee2024}.
65
+
66
+ \subsection{Historical context and method}
67
+
68
+ Metric \(k\)-median has been a testing ground for LP rounding,
69
+ primal-dual algorithms, and local search. Charikar, Guha, Tardos and
70
+ Shmoys gave the first constant-factor approximation through LP
71
+ rounding~\cite{CharikarGuhaTardosShmoys2002}. Jain and
72
+ Vazirani connected the cardinality constraint with metric facility
73
+ location through Lagrangian relaxation and the primal-dual
74
+ method~\cite{JainVazirani2001}. The combinatorial improvements of
75
+ Charikar and Guha~\cite{CharikarGuha1999} and the greedy dual-fitting
76
+ approach of Jain et al.~\cite{JainEtAl2003} developed this connection
77
+ further. A different route, the bounded-swap local search of Arya et
78
+ al.~\cite{Arya2004}, achieves factor \(3+\varepsilon\).
79
+
80
+ Li and Svensson~\cite{LiSvensson2016} made constant-additive
81
+ pseudo-approximations a route past the factor-three barrier: a constant
82
+ number of extra facilities can be removed at an arbitrarily small
83
+ additional approximation loss. Subsequent bi-point rounding, including
84
+ the corrected \(2.675+\varepsilon\) guarantee of Byrka et
85
+ al.~\cite{ByrkaEtAl2017}, refined this approach. Gowda et
86
+ al.~\cite{GowdaEtAl2023} obtained \(2.613\) in their SODA 2023 version.
87
+ Cohen-Addad et al.~\cite{CGLSS2026} reached
88
+ \(2+\varepsilon\), first announced in 2025. Byrka et
89
+ al.~\cite{ByrkaEtAl2026} subsequently developed a graph-based iterative
90
+ rounding framework that also gives \(2+\varepsilon\) for metric
91
+ \(k\)-median and extends to other clustering objectives.
92
+ Theorem~\ref{thm:main} reaches every fixed factor above the
93
+ \(1+2/e\) hardness boundary in the general candidate-facility model.
94
+
95
+ Our construction follows the iterative graph framework, with the
96
+ cost analysis replaced by a directed comparison inequality and a
97
+ potential that retains some surviving assignments after an opening.
98
+ The earlier framework's general transfer theorem uses a parameter at
99
+ least \(2\) in the metric \(k\)-median case
100
+ \cite[Theorem~6.1]{ByrkaEtAl2026}; it does not supply the smaller factor
101
+ proved here. We establish the grid preparation, physical updates,
102
+ comparison, and deterministic implementation together.
103
+
104
+ A separate companion combines anchor recovery with bounded-price payment
105
+ accounting to give an independent randomized approximation below factor
106
+ \(2\) while respecting the facility budget~\cite[Theorem~1.2]{OpenAIRecovery2026}.
107
+
108
+ Two other methodological antecedents are useful to distinguish.
109
+ Splitting fractional facilities and organizing assignments around
110
+ separated representatives and bundles are standard LP-rounding
111
+ techniques; Charikar and Li~\cite{CharikarLi2012} provide a close
112
+ predecessor. The pair updates used in our preparation belong to the
113
+ dependent-rounding approach of Srinivasan~\cite{Srinivasan2001} and
114
+ Gandhi et al.~\cite{GandhiEtAl2006}, with weighted variants studied by
115
+ Byrka et al.~\cite{ByrkaEtAl2017}. We prove the particular moment bounds
116
+ and coupled supplier construction needed here. Likewise, reducing the
117
+ support of a distribution while matching moments is a standard
118
+ Carath\'eodory argument; see Bayer and Teichmann~\cite{BayerTeichmann2005}
119
+ for the finite-cubature perspective. Our implementation specifies which
120
+ moments suffice throughout the physical process and proves the required
121
+ rational encoding bounds.
122
+
123
+ \subsection{Proof overview}
124
+
125
+ The proof separates the preparation of fractional openings, their
126
+ iterative rounding, and the removal of randomness and surplus. The
127
+ intermediate guarantee is measured against the standard assignment LP:
128
+ its variable \(y_i\) is the amount of opening at facility \(i\), and each
129
+ client receives a unit of this opening mass. The LP has total opening
130
+ mass at most \(k\) and cost at most \(\OPT_k\).
131
+
132
+ \paragraph{Preparing a constant grid.}
133
+ Section~\ref{sec:preparation} replaces the LP openings by multiples of
134
+ \(g=1/\Delta\), where the even integer \(\Delta\) depends only on the
135
+ accuracy. The total mass increases by at most \(3g\), and each client's
136
+ expected assignment cost increases by an arbitrarily small factor.
137
+ Separated representative clients define disjoint bundles of nearby
138
+ opening mass. A bundle's deficit is the part missing from a unit; its
139
+ suppliers are the facilities or other bundles holding that part of the
140
+ representative's assignment. Rounding deficits together with their
141
+ suppliers controls both the opening budget and the cost of restoring a
142
+ full unit. This coupling must allow one supplier to serve many clients,
143
+ because assignment mass is not a shared capacity.
144
+
145
+ \paragraph{Rounding the grid.}
146
+ View every positive grid opening as copies of mass \(g\). In each round,
147
+ a directed graph specifies which copies a source erases when that source's
148
+ facility opens. Each target has exactly \(\Delta\) incoming sources,
149
+ chosen with distance-dependent probabilities. Opening and erasing are
150
+ balanced so that only a constant additional number of facilities is
151
+ needed. This source-opening and neighbor-erasure framework, including
152
+ balanced batches and forced large updates, builds on Byrka et
153
+ al.~\cite[Sections~3--6]{ByrkaEtAl2026}.
154
+
155
+ The connection-cost analysis needs a different comparison below factor
156
+ two. For each client, we track surviving copies from its initial assigned
157
+ unit and a persistent bound on its eventual connection distance. A
158
+ potential combines their remaining assignment cost with that bound. Its
159
+ coefficient depends on elapsed time as well as surviving mass. When one
160
+ of the client's own copies opens, we continue tracking the cheaper
161
+ survivors; this produces a subtraction that pays for other possible
162
+ erasures. The finite inequality in Section~\ref{sec:inequality} captures
163
+ that payment for arbitrary directed comparison coefficients. Its proof
164
+ transfers contributions from positive rows to lower-distance rows, whose
165
+ negative contributions cover them. Appendix~\ref{app:certificates}
166
+ proves every scalar estimate by explicit rational polynomial certificates.
167
+ The geometric substitution and the potential analysis are given in
168
+ Section~\ref{sec:rounding}.
169
+
170
+ A source erasing many copies is handled by forcing its facility open.
171
+ Because this choice depends on the graph, its potential change is bounded
172
+ for each realized graph first. Only then do we average over graphs. This
173
+ order lets the finite directed inequality control the averaged drift
174
+ without conditioning on a graph-dependent forcing event.
175
+
176
+ \paragraph{A deterministic solution and the exact budget.}
177
+ The preceding analysis uses randomness, but only specified low-order
178
+ moments of each local choice enter its bounds. Section~\ref{sec:derandomization}
179
+ constructs polynomial-size rational distributions preserving these
180
+ moments. All physical histories are expanded for a constant number of
181
+ rounds, and the cheapest output satisfying the additive budget is chosen.
182
+ The separate rational-arithmetic analysis proves polynomial time in the
183
+ binary input length. The result is a deterministic approximation opening
184
+ at most \(k+c\) facilities for an accuracy-dependent constant \(c\).
185
+ Li and Svensson's reduction then removes this surplus with an arbitrarily
186
+ small additional loss.
187
+
188
+ \paragraph{Organization.}
189
+ Section~\ref{sec:preliminaries} fixes the model and states the external
190
+ additive-to-ordinary reduction. Section~\ref{sec:preparation} prepares the
191
+ openings. Section~\ref{sec:inequality} proves the finite drift inequality,
192
+ with its scalar certificates in Appendix~\ref{app:certificates}.
193
+ Section~\ref{sec:rounding} gives and analyzes the iterative procedure.
194
+ Section~\ref{sec:derandomization} supplies the deterministic implementation
195
+ and completes the proof of Theorem~\ref{thm:main}.
196
+
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/preliminaries.tex ADDED
@@ -0,0 +1,104 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Preliminaries and the reduction}\label{sec:preliminaries}
2
+
3
+ We use the client set \(J\), candidate set \(F\), connection cost
4
+ \(\cost\), and optimum \(\OPT_k\) defined in the introduction.
5
+ Polynomial time includes the binary encodings of all distances.
6
+ We henceforth assume \(J\ne\varnothing\) and \(1\le k\le |F|\).
7
+ This section fixes the fractional representation and states the external
8
+ reduction that will remove the final constant additive surplus.
9
+
10
+ \subsection{The fractional solution}
11
+
12
+ We use the standard relaxation
13
+ \begin{equation}\label{eq:lp}
14
+ \begin{aligned}
15
+ \text{minimize}\quad &\sum_{j\in J}\sum_{i\in F}d(j,i)x_{ij}\\
16
+ \text{subject to}\quad&
17
+ \sum_{i\in F}x_{ij}=1 &&(j\in J),\\
18
+ &0\le x_{ij}\le y_i\le1 &&(i\in F,\ j\in J),\\
19
+ &\sum_{i\in F}y_i\le k.
20
+ \end{aligned}
21
+ \end{equation}
22
+ Its rational optimum can be found in polynomial time. For fixed openings
23
+ \(y_i\), assign each client to its nearest unit of opening mass, using a fixed
24
+ order to break ties. If \(h_j(t)\) is the distance needed to accumulate mass
25
+ \(t\), put
26
+ \[
27
+ V_j=\int_0^1h_j(t)\,dt.
28
+ \]
29
+ Then \(L=\sum_jV_j\le\OPT_k\) for an optimal solution of~\eqref{eq:lp}.
30
+
31
+ As in LP-rounding constructions such as Charikar--Li~\cite[Section~2]{CharikarLi2012},
32
+ it is convenient to split an opening into co-located pieces so that each
33
+ client's nearest-unit assignment uses whole pieces. There are only
34
+ polynomially many needed split points: each client uses at most one partial
35
+ piece in a fixed distance order. Refine each facility simultaneously at all
36
+ the resulting cut points. Denote the whole-piece assignment of client \(j\)
37
+ by \(F_j\). For a set \(U\) of pieces, write \(y(U)=\sum_{i\in U}y_i\);
38
+ thus \(y(F_j)=1\) and \(V_j=\sum_{i\in F_j}y_id(j,i)\).
39
+
40
+ Internal pieces at one location are allowed to be distinct, so their distance
41
+ can be zero. All geometric arguments use only nonnegativity, symmetry, and
42
+ the triangle inequality. Whenever a procedure returns open pieces, merge
43
+ them by their original facility identity. Merging preserves every client's
44
+ connection cost and cannot increase the number of facilities.
45
+
46
+ \subsection{Constant-additive pseudo-approximation}
47
+
48
+ \begin{definition}
49
+ A \(c\)-additive \(\alpha\)-approximation for metric \(k\)-median returns
50
+ at most \(k+c\) facilities of cost at most \(\alpha\OPT_k\).
51
+ The additive allowance \(c\) is independent of the input instance.
52
+ \end{definition}
53
+
54
+ We use the following established result.
55
+
56
+ \begin{theorem}[Li--Svensson~\cite{LiSvensson2016}, Theorem~4 of the 2014 manuscript]
57
+ \label{thm:li-svensson}
58
+ Let \(\alpha>1\), and suppose \(\mathcal A\) is a \(c\)-additive
59
+ \(\alpha\)-approximation algorithm for metric \(k\)-median.
60
+ For every \(\eta>0\), there is an ordinary
61
+ \((\alpha+\eta)\)-approximation algorithm with running time
62
+ \(n^{O(c/\eta)}\) times the running time of \(\mathcal A\).
63
+ For fixed \(\alpha,c,\eta\), this is polynomial overhead.
64
+ \end{theorem}
65
+
66
+ The theorem permits separate client and candidate sets and applies the
67
+ pseudo-algorithm to restricted candidate instances. Our construction works
68
+ on every such instance. We will obtain a deterministic pseudo-algorithm
69
+ before applying Theorem~\ref{thm:li-svensson}; the external reduction is not
70
+ being used to convert an expected-cost statement into determinism.
71
+
72
+ For each fixed accuracy we permit all grid denominators, numbers of rounds,
73
+ and additive allowances to be constants of any size. They may depend on
74
+ that accuracy, but not on \(k\), the number of input points, their distances,
75
+ or their bit lengths. Thus it suffices to prove, for each fixed
76
+ \(\tau>0\), a deterministic \(c_\tau\)-additive
77
+ \((1+2/e+\tau)\)-approximation. Our analysis in fact bounds the
78
+ pseudo-solution against \(L\), the initial fractional cost. This does not
79
+ assert the same factor for rounding the original relaxation to exactly
80
+ \(k\) facilities: the additive allowance and the subsequent reduction
81
+ are essential.
82
+
83
+ \subsection{Probability and bookkeeping}
84
+
85
+ We use \(\E\), \(\Prob\), and \(\Var\) for expectation, probability, and variance.
86
+ Every distribution used below has finite support. Randomized procedures
87
+ first provide the estimates; Section~\ref{sec:derandomization} replaces their
88
+ choices by explicit polynomial-size lists.
89
+
90
+ Two elementary facts will be used repeatedly. First, for a nonnegative random
91
+ cost \(C\) and an event \(E\) of probability at least \(1-\rho>0\),
92
+ \begin{equation}\label{eq:conditioning}
93
+ \E[C\mid E]\le\frac{\E C}{1-\rho}.
94
+ \end{equation}
95
+ No cost--event independence is required. Second, a finite distribution
96
+ contains an outcome whose cost is at most its expected cost. These facts
97
+ allow us to discard budget failures and select a single output by total
98
+ cost; we never require all individual client expectation bounds to hold
99
+ simultaneously at that output.
100
+
101
+ The notation \(O_\Delta(\cdot)\) means that its implicit constant may depend
102
+ on the fixed grid denominator \(\Delta\), and on no input parameter.
103
+ All unqualified constants in the geometric and analytic estimates are
104
+ absolute, unless an explicit previously fixed parameter is indicated.
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/preparation.tex ADDED
@@ -0,0 +1,526 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Preparing the openings}\label{sec:preparation}
2
+
3
+ We first put the fractional openings on a sufficiently fine constant grid.
4
+ The use of separated representatives and bundles is motivated by the
5
+ discretization approach in~\cite{ByrkaEtAl2026}. The construction below
6
+ rounds a bundle's missing assignment mass together with the facilities
7
+ that can supply it. This coupling provides both an additive opening
8
+ bound and a multiplicative connection-cost bound.
9
+
10
+ Throughout this Section, the client set is nonempty; an instance without
11
+ clients requires no cost analysis. We start with feasible fractional
12
+ openings $0\le y_i\le1$. For each client $j$, choose a nearest-unit
13
+ assignment $x_{ij}$, resolving ties in a fixed order, and write
14
+ \[
15
+ V_j=\sum_i d(i,j)x_{ij}.
16
+ \]
17
+ The feasibility constraints are $\sum_i x_{ij}=1$ and $x_{ij}\le y_i$;
18
+ there is no supply constraint shared by different clients.
19
+
20
+ \begin{theorem}\label{thm:preparation}
21
+ For every $\eta>0$, there is a constant $\Delta_0$ with the following
22
+ property. Given a finite rational metric instance and feasible rational
23
+ openings $0\le y_i\le1$ with a nearest-unit assignment of cost $V_j$
24
+ for each client $j$, fix any constant even integer $\Delta\ge\Delta_0$ and let
25
+ $g=1/\Delta$. There is a randomized procedure, running in expected
26
+ polynomial time on rational inputs, that produces openings
27
+ $\widetilde y_i\in[0,1]\cap g\mathbb Z$, allowing polynomially many
28
+ co-located labeled facility pieces, such that
29
+ \[
30
+ 1\le\sum_i\widetilde y_i\le\sum_i y_i+3g
31
+ \]
32
+ for every output, and the expected nearest-unit assignment cost of every
33
+ client $j$ is at most $(1+\eta)V_j$.
34
+ In particular the grid can be required to satisfy any additional
35
+ positive instance-independent upper bound on $g$.
36
+ \end{theorem}
37
+
38
+ The expectation in Theorem~\ref{thm:preparation} is taken after rejecting
39
+ outcomes that exceed the opening budget. Section~\ref{sec:derandomization}
40
+ gives a deterministic implementation that preserves the corresponding
41
+ bound on the sum of the client costs.
42
+
43
+ We use the following elementary dependent-rounding observation, in both
44
+ weighted and unweighted form. The mean-preserving pair update and its
45
+ product-supermartingale argument follow the standard
46
+ approach~\cite{Srinivasan2001,GandhiEtAl2006}; weighted rounding with one
47
+ residual fraction is also studied in~\cite[Section~2]{ByrkaEtAl2017}.
48
+ We give the proof to specify exactly the moment guarantees used here.
49
+
50
+ \begin{lemma}\label{lem:prep-weighted-rounding}
51
+ Let $q_e\ge0$ be rational counts and let $\beta_e>0$ be rational weights.
52
+ One can randomly update the counts within the bounds
53
+ $[\lfloor q_e\rfloor,\lceil q_e\rceil]$, preserving
54
+ $\sum_e\beta_e q_e$ on every update, until at most one count is
55
+ fractional. Every first moment is preserved, and the expectation of
56
+ every product of two distinct counts is at most the product of their
57
+ initial values. Rounding the possible remaining fractional count with
58
+ its correct mean preserves these moment assertions.
59
+ For the resulting integer counts $Q_e$,
60
+ \[
61
+ \Var(Q_e)\le q_e,\qquad
62
+ \E[Q_eQ_f]\le q_eq_f\quad(e\ne f).
63
+ \]
64
+ The procedure uses linearly many two-coordinate updates.
65
+ \end{lemma}
66
+
67
+ \begin{proof}
68
+ When two coordinates are fractional, move them along the line
69
+ \[
70
+ (q_e,q_f)\longmapsto
71
+ (q_e+t,q_f-(\beta_e/\beta_f)t)
72
+ \]
73
+ to one of the two endpoints allowed by their fixed floor and ceiling
74
+ bounds. Choose the endpoint probabilities so that the conditional
75
+ mean of $t$ is zero. At least one coordinate becomes integral, and
76
+ integral coordinates are not updated subsequently. Each coordinate
77
+ is a martingale. The product of the two updated coordinates is a
78
+ concave quadratic in $t$; a product involving exactly one updated
79
+ coordinate has unchanged conditional mean. Thus every distinct-pair
80
+ product is a supermartingale. Rounding the last fractional coordinate
81
+ with the correct conditional mean leaves all these products unchanged
82
+ in expectation. Finally, an integer random variable supported on
83
+ $\{m,m+1\}$, with mean $m+\theta$, has variance
84
+ $\theta(1-\theta)\le m+\theta$. This proves the variance assertion.
85
+ \end{proof}
86
+
87
+ \begin{proof}[Proof of Theorem~\ref{thm:preparation}]
88
+ We first form disjoint bundles containing most of each representative's
89
+ assigned mass. We then round their deficits jointly with the openings
90
+ that supply them, reserving a small amount of budget for clipping large
91
+ deficits. After rounding inside bundles, every representative can again
92
+ receive one unit. The final part of the proof compares connection costs
93
+ at two representative-distance scales and conditions on the budget event.
94
+
95
+ We will choose positive rational constants in the order
96
+ \[
97
+ \delta,\quad M,\quad T_1,\quad\gamma,\quad g,
98
+ \]
99
+ with $\delta$ small, $M$ and then $T_1$ large, and $\gamma$ and then $g$
100
+ small. All choices depend only on $\eta$; the last choice means that
101
+ every sufficiently fine even grid is permitted. During the proof we
102
+ require
103
+ \begin{equation}\label{eq:prep-parameter-basics}
104
+ 0<\delta\le\tfrac14,\qquad 0<\gamma\le1,\qquad
105
+ \theta:=\frac1{M\delta}\le\tfrac18,\qquad
106
+ \alpha:=\frac M{\delta T_1}\le\tfrac14.
107
+ \end{equation}
108
+ Set $p_0=1-\theta$ and $\beta=M/T_1=\delta\alpha$.
109
+
110
+ \paragraph{Splitting and representatives.}
111
+ For each original facility, view its opening $y_i$ as an interval of
112
+ length $y_i$ and its assignment to client $j$ as the initial subinterval
113
+ of length $x_{ij}$. Split at the endpoints of these subintervals for all
114
+ clients. There are at most $|J|+1$ positive-mass pieces per original
115
+ facility, and every assignment now uses whole pieces. Retain the
116
+ notation $y_i$ for the mass of a piece, and let $F_j$ be the set of pieces
117
+ used by client $j$. Thus
118
+ \[
119
+ y(F_j)=1,\qquad
120
+ V_j=\sum_{i\in F_j}y_i d(i,j),\qquad
121
+ y(W):=\sum_{i\in W}y_i.
122
+ \]
123
+ Pieces retain the distances of their original facility. They may be
124
+ treated as distinct candidates throughout the rounding; merging
125
+ co-located integral openings at the end preserves all connection
126
+ distances and can only decrease the number of opened facilities.
127
+
128
+ Process the clients in nondecreasing order of $V_j$. Select each
129
+ remaining client $s$ as a representative and absorb every remaining
130
+ client $j$ for which $d(j,s)\le MV_j$. Write $\mathcal S$ for the set of
131
+ representatives. A client $j$ assigned to $s$ satisfies
132
+ \begin{equation}\label{eq:prep-representative-properties}
133
+ V_s\le V_j,\qquad d(j,s)\le MV_j.
134
+ \end{equation}
135
+ Distinct representatives satisfy
136
+ \[
137
+ d(s,t)>M\max(V_s,V_t):
138
+ \]
139
+ indeed, the later one was not absorbed by the earlier one. Let $L_s$ be
140
+ the distance to a nearest other representative, taking $L_s=\infty$
141
+ when $s$ is the only representative. Define
142
+ \[
143
+ P_s=\{i\in F_s:d(s,i)\le\delta L_s\},\quad
144
+ p_s=y(P_s),\quad c_s=1-p_s,\quad A_s=F_s\setminus P_s,
145
+ \]
146
+ and let $U$ consist of all pieces outside $\bigcup_s P_s$.
147
+ For $L_s=\infty$, interpret $P_s=F_s$ and $c_s=0$.
148
+
149
+ The bundles $P_s$ are disjoint. Otherwise a piece in $P_s\cap P_t$
150
+ would imply
151
+ \[
152
+ d(s,t)\le\delta(L_s+L_t)\le2\delta d(s,t),
153
+ \]
154
+ which is impossible. For finite $L_s$, the mass in $A_s$ has distance
155
+ at least $\delta L_s$ from $s$, so
156
+ \begin{equation}\label{eq:prep-deficit-small}
157
+ \delta L_s c_s\le V_s,\qquad
158
+ 0\le c_s\le\theta,\qquad p_s\ge p_0.
159
+ \end{equation}
160
+ These bounds also cover $V_s=0$: in that case $c_s=0$.
161
+
162
+ \paragraph{Supplier stars and signed counts.}
163
+ For the raw opening count, give every bundle a base level of one. A
164
+ supplier star couples planned deficits in its target bundles to the
165
+ mass that will supply them. One planned count unit subtracts mass $g$
166
+ from each target bundle and adds mass $g$ at the supplier if it lies in $U$.
167
+ A bundle supplier incurs no additional opening in this accounting.
168
+ Thus a star with $d$ targets changes the opening mass by $(1-d)g$ for
169
+ an outside supplier and by $-dg$ for a bundle supplier.
170
+
171
+ Make a list $\mathcal E$ of stars; a star $e$ has weight $w_e$, a flag
172
+ $a_e\in\{0,1\}$ indicating an outside supplier, a target set
173
+ $D_e\subseteq\mathcal S$, and a specified supplier:
174
+ \begin{enumerate}
175
+ \item For each $i\in U$, take $w_e=y_i$, $a_e=1$,
176
+ $D_e=\{s:i\in A_s\}$, and supplier $i$.
177
+ \item For each pair $s,t$ with $y(A_s\cap P_t)>0$, take
178
+ $w_e=y(A_s\cap P_t)$, $a_e=0$, $D_e=\{s\}$, and supplier $P_t$.
179
+ Necessarily $t\ne s$.
180
+ \item For each $s$ with $c_s>0$, take $w_e=\gamma c_s$, $a_e=0$,
181
+ $D_e=\{s\}$, and use as supplier the bundle of a nearest other
182
+ representative. Such a representative exists because $c_s>0$.
183
+ \end{enumerate}
184
+ The last stars are called extra stars. The planned count of star $e$
185
+ is $q_e=w_e/g$. With $u_e=a_e-|D_e|$, the planned raw opening mass is
186
+ \begin{equation}\label{eq:prep-raw-identity}
187
+ |\mathcal S|+\sum_e u_e w_e
188
+ =\sum_i y_i-\gamma\sum_s c_s.
189
+ \end{equation}
190
+ To see this, the flag-one weights sum to $y(U)$, while the total weight
191
+ targeting $s$ is $(1+\gamma)c_s$.
192
+
193
+ Apply Lemma~\ref{lem:prep-weighted-rounding} independently to the
194
+ positive and negative signs of $u_e$, using weights $|u_e|$. Complete
195
+ the rounding of the positive class by rounding its possible last
196
+ fraction with the correct mean. Round the zero-coefficient counts
197
+ independently between their floor and ceiling. Leave the last
198
+ fractional count of the negative class, if any, temporarily unrounded.
199
+ All counts are then integral except possibly this one.
200
+
201
+ If there is no remaining fraction, the resulting counts are both the
202
+ nominal counts and the actual activation counts. Otherwise, write the
203
+ remaining count as $m+\xi$, where $0<\xi<1$, and let its star have
204
+ $d=|D_e|$ targets. Its nominal count is $m+\operatorname{Bernoulli}(\xi)$.
205
+ If its flag is one, open $(m+1)g$ at its supplier, irrespective of the
206
+ nominal coin. Activate $m$ units at each target, and activate one
207
+ additional unit at every target in a random subset of size
208
+ \[
209
+ H\in\{\lfloor d\xi\rfloor,\lceil d\xi\rceil\},
210
+ \qquad \E H=d\xi,
211
+ \]
212
+ whose membership marginal is $\xi$ at every target. Such a subset is
213
+ obtained by choosing the indicated size with the correct mean and
214
+ then taking a uniformly shifted interval of that size in a fixed
215
+ cyclic ordering of the targets. The nominal coin can be independent
216
+ of this choice. All other stars use their integral counts for both
217
+ openings and activations.
218
+
219
+ This modification bounds the raw opening error independently of the
220
+ number of targets. For the exceptional star its actual signed
221
+ contribution, in count units, minus its planned contribution is
222
+ \[
223
+ a_e(m+1)-dm-H-(a_e-d)(m+\xi)
224
+ =a_e(1-\xi)+d\xi-H<2.
225
+ \]
226
+ A positive coefficient $u_e$ necessarily equals one, so the last
227
+ rounding in the positive class adds less than one further count unit.
228
+ The zero class has no signed contribution. If $\widetilde y_i$ denotes
229
+ the actual opening on $U$, and $Z_s$ denotes the total activated deficit
230
+ mass at $s$, we therefore have on every outcome
231
+ \begin{equation}\label{eq:prep-raw-bound}
232
+ \sum_{i\in U}\widetilde y_i+\sum_s(1-Z_s)
233
+ \le\sum_i y_i-\gamma\sum_s c_s+3g.
234
+ \end{equation}
235
+ Moreover, each actual outside opening dominates both its nominal
236
+ opening and every activation demand placed on it by a single target.
237
+
238
+ \paragraph{Deficit moments and clipping.}
239
+ The signed count already controls raw opening mass. The remaining
240
+ obstacle is that an activated deficit might leave too little mass in its
241
+ own bundle. We cap that deficit and pay for the added bundle mass with
242
+ the reserve in Equation~\ref{eq:prep-raw-bound}.
243
+ For every $s$, let $A_{es}$ be the integer activation count from a star
244
+ targeting $s$. Then
245
+ \begin{equation}\label{eq:prep-deficit-moments}
246
+ \E Z_s=(1+\gamma)c_s,
247
+ \qquad \Var(Z_s)\le g(1+\gamma)c_s.
248
+ \end{equation}
249
+ Here it matters that the last negative star may depend on the preceding
250
+ random choices. Condition on the complete count vector immediately
251
+ before its exceptional rounding. At most one coordinate is
252
+ fractional, so for distinct $e,f$ targeting $s$, at least one of
253
+ $A_{es},A_{fs}$ is deterministic under this conditioning. Each has
254
+ conditional mean equal to its current count. Their conditional product
255
+ expectation is therefore the product of those two current counts.
256
+ The distinct-pair product bound in
257
+ Lemma~\ref{lem:prep-weighted-rounding} consequently still holds for
258
+ these activations. Their individual means are $q_e$, and each is
259
+ supported on $\{\lfloor q_e\rfloor,\lceil q_e\rceil\}$. Thus
260
+ \[
261
+ \Var(Z_s)
262
+ \le g^2\sum_{e:s\in D_e}\Var(A_{es})
263
+ \le g^2\sum_{e:s\in D_e}q_e
264
+ =g(1+\gamma)c_s,
265
+ \]
266
+ as asserted. The nominal counts also retain the same first and
267
+ distinct-pair moment bounds.
268
+
269
+ Clip the deficit at one half:
270
+ \[
271
+ Z_s^*=\min(Z_s,\tfrac12),\qquad p'_s=1-Z_s^*.
272
+ \]
273
+ Discard any excess activation units. This can be done in whole units
274
+ because $\Delta$ is even. By Equation~\ref{eq:prep-parameter-basics},
275
+ $\mu_s:=\E Z_s\le1/4$. For any random variable $X$ with mean $\mu<b$,
276
+ \[
277
+ (X-b)_+\le\frac{(X-\mu)^2}{b-\mu}.
278
+ \]
279
+ Indeed the assertion is immediate when $X\le b$, and otherwise follows
280
+ by expanding $(X-\mu)^2=(X-b+b-\mu)^2$.
281
+ Equation~\ref{eq:prep-deficit-moments} therefore gives
282
+ \[
283
+ \E(Z_s-\tfrac12)_+\le4g(1+\gamma)c_s.
284
+ \]
285
+ Let $\mathcal G$ be the event that
286
+ \[
287
+ \sum_s(Z_s-Z_s^*)\le\gamma\sum_s c_s.
288
+ \]
289
+ If some $c_s$ is positive, Markov's inequality gives
290
+ \begin{equation}\label{eq:prep-budget-probability}
291
+ \Prob(\mathcal G)\ge1-\rho,
292
+ \qquad \rho:=\frac{4g(1+\gamma)}\gamma.
293
+ \end{equation}
294
+ If all $c_s$ vanish, all activations and discarded amounts are zero,
295
+ and $\mathcal G$ holds surely. Equations~\ref{eq:prep-raw-bound} and
296
+ \ref{eq:prep-budget-probability} show that a vector with bundle sums
297
+ $p'_s$ has total opening mass at most $\sum_i y_i+3g$ on $\mathcal G$.
298
+
299
+ \paragraph{Rounding within bundles and supplying one unit.}
300
+ Condition on the complete star-rounding outcome, including the retained
301
+ activations. In each bundle independently, rescale piece $i\in P_s$ to
302
+ mass
303
+ \[
304
+ \overline y_i=y_i\frac{p'_s}{p_s}.
305
+ \]
306
+ Since $y_i\le p_s$ and $1/2\le p'_s\le1$, these masses belong to $[0,1]$.
307
+ Their sum $p'_s$ is a grid multiple. Apply the unweighted version of
308
+ Lemma~\ref{lem:prep-weighted-rounding} to counts $\overline y_i/g$.
309
+ The preserved sum is integral in count units, so there is no final
310
+ fraction. This produces grid masses $\widetilde y_i$ with conditional
311
+ means $\overline y_i$ and nonpositive conditional pair covariances.
312
+ All masses remain at most one, because one is a grid point. Likewise
313
+ the outside opening at a piece of original mass $y_i$ is at most
314
+ $g\lceil y_i/g\rceil\le1$, even under the exceptional correction.
315
+
316
+ Every representative $s$ can now receive one unit: take its entire
317
+ bundle mass $p'_s$ and supply its retained deficit $Z_s^*$ using the
318
+ retained activations. Each outside supplier has enough mass for its
319
+ activation demand at $s$. Any bundle supplier is different from $P_s$.
320
+ The total demand of $s$ on any one such bundle is at most its entire
321
+ retained deficit, hence at most $1/2$, while every supplying bundle has
322
+ mass at least $1/2$. Allocate this demand greedily over its pieces.
323
+ The bundles and $U$ are disjoint, and different clients have separate
324
+ assignment constraints. This proves feasibility for each client
325
+ individually, even before conditioning on $\mathcal G$. It also shows
326
+ that the total opening mass is at least one.
327
+
328
+ \paragraph{Cost comparison at a distant representative scale.}
329
+ Fix a client $j$ and its representative $s$, and put $D=d(j,s)$.
330
+ Let $R_s=\max_{i\in F_s}d(s,i)$, and define the radius
331
+ \[
332
+ K_s=\begin{cases}L_s,&c_s>0,\\R_s,&c_s=0.\end{cases}
333
+ \]
334
+ If $V_j=0$, Equation~\ref{eq:prep-representative-properties} gives
335
+ $D=V_s=0$. All pieces of $F_s$ then have distance zero from $j$,
336
+ $c_s=0$, and $Z_s=0$ surely. The rounded bundle $P_s=F_s$ still has
337
+ one unit at distance zero. Hence the new cost is identically zero.
338
+ We may therefore assume $V_j>0$ in the remaining cost analysis.
339
+
340
+ Suppose first that $K_s>T_1V_j$. We have $R_s\ge\delta K_s$: this is
341
+ immediate if $c_s=0$, and otherwise some assigned mass lies beyond
342
+ $\delta L_s$. Consequently $D/R_s\le\alpha<1$. This controls the
343
+ cost of exchanging the portions of $F_j$ and $F_s$ that are not shared.
344
+ Leave the shared pieces matched identically. The masses of
345
+ $F_s\setminus F_j$ and $F_j\setminus F_s$ are equal. Each piece in the
346
+ former set is at distance at most $R_s+D$ from $j$. Each piece in the
347
+ latter set is at distance at least $R_s-D$ from $j$, because the
348
+ nearest-unit assignment at $s$ uses all closer mass before stopping at
349
+ radius $R_s$. This argument remains valid at ties. Comparing the two
350
+ residual costs shows that using the old assignment $F_s$ for client $j$
351
+ has cost at most
352
+ \begin{equation}\label{eq:prep-far-exchange}
353
+ C_j(F_s):=\sum_{i\in F_s}y_i d(j,i)
354
+ \le\frac{1+\alpha}{1-\alpha}V_j.
355
+ \end{equation}
356
+
357
+ Serve $j$ with the feasible assignment just constructed for $s$.
358
+ For each $i\in P_s$,
359
+ \[
360
+ \E\widetilde y_i
361
+ =y_i\E[p'_s]/p_s\le y_i/p_s.
362
+ \]
363
+ For an ordinary star, the expected retained activation mass is at most
364
+ its original weight. Thus outside suppliers do not increase their
365
+ expected cost charge. It remains to compare arbitrary new supply
366
+ inside a bundle $P_t$ with the old pieces in $A_s\cap P_t$.
367
+ This case only arises when $c_s>0$. Then $D\le\beta L_s$, and for any
368
+ old supplier piece $i\in P_t$,
369
+ \[
370
+ d(j,i)\ge d(s,t)-D-\delta L_t
371
+ \ge(1-\beta-\delta)d(s,t).
372
+ \]
373
+ Any two pieces of $P_t$ are at distance at most $2\delta L_t$.
374
+ Because $L_t\le d(s,t)$ and $1-\beta-\delta>0$, every possible new
375
+ supplier piece has distance to $j$ at most
376
+ \[
377
+ \kappa\,d(j,i),\qquad
378
+ \kappa:=1+\frac{2\delta}{1-\beta-\delta}.
379
+ \]
380
+ The comparison holds for every old piece, so it also holds relative to
381
+ the weighted mean distance of the old pieces aggregated by that star.
382
+ Multiplying by its expected retained activation mass bounds its
383
+ expected cost by $\kappa$ times its old cost contribution.
384
+
385
+ Finally, for the extra star at $s$, its supplier $P_t$ satisfies
386
+ $d(s,t)=L_s$ and $L_t\le L_s$. Every supply position is therefore at
387
+ distance at most $(\beta+1+\delta)L_s$ from $j$. By
388
+ Equation~\ref{eq:prep-deficit-small}, its expected cost is at most
389
+ \[
390
+ (\beta+1+\delta)\gamma c_s L_s
391
+ \le\frac{(\beta+1+\delta)\gamma}{\delta}V_j.
392
+ \]
393
+ There is no extra star when $c_s=0$.
394
+ Combining these bounds with Equation~\ref{eq:prep-far-exchange}, the
395
+ unconditional expected nearest-unit cost in this case is at most
396
+ $B_{\mathrm{far}}V_j$, where
397
+ \begin{equation}\label{eq:prep-far-factor}
398
+ B_{\mathrm{far}}
399
+ :=\max\{p_0^{-1},\kappa\}\frac{1+\alpha}{1-\alpha}
400
+ +\frac{(\beta+1+\delta)\gamma}{\delta}.
401
+ \end{equation}
402
+
403
+ \paragraph{Cost comparison at a nearby representative scale.}
404
+ Now suppose $K_s\le T_1V_j$. Consider the mass on the old set $F_j$,
405
+ using nominal rounded masses on $U$ and actual rounded masses in the
406
+ bundles. This mass is available in the actual opening vector. Its
407
+ unconditional expected cost is at most $V_j/p_0$: nominal outside
408
+ openings have mean $y_i$, and a bundle piece has expected mass at most
409
+ $y_i/p_s\le y_i/p_0$.
410
+
411
+ We bound the expected shortfall of this available mass from one.
412
+ Write $M_U$ for its nominal mass on $U\cap F_j$. The first and pair
413
+ moments of the nominal counts imply
414
+ \begin{equation}\label{eq:prep-outside-noise}
415
+ \E M_U=y(U\cap F_j),\qquad
416
+ \Var(M_U)\le g\,y(U\cap F_j)\le g.
417
+ \end{equation}
418
+ For a fixed complete star outcome, put
419
+ \[
420
+ a_t=y(F_j\cap P_t),\qquad
421
+ \overline M_P=\sum_t a_t p'_t/p_t,
422
+ \]
423
+ and write $M_P$ for the actual rounded mass on these bundle pieces.
424
+ Conditional on the star outcome, bundle rounding has nonpositive pair
425
+ covariances within each bundle and is independent between bundles.
426
+ The variance of a single grid-rounded mass of conditional mean
427
+ $\overline y_i$ is at most $g\overline y_i$. Therefore
428
+ \begin{equation}\label{eq:prep-conditional-noise}
429
+ \E[M_P\mid\text{star outcome}]=\overline M_P,\qquad
430
+ \Var(M_P\mid\text{star outcome})
431
+ \le g\overline M_P\le g/p_0.
432
+ \end{equation}
433
+
434
+ Clipping at $1/2$ cannot increase distance from $c_t\le1/2$, so
435
+ Equation~\ref{eq:prep-deficit-moments} gives
436
+ \begin{align}
437
+ \E|p'_t-p_t|
438
+ &=\E|c_t-Z_t^*|\notag\\
439
+ &\le\E|c_t-Z_t|
440
+ \le\gamma c_t+\sqrt{g(1+\gamma)c_t}.
441
+ \label{eq:prep-rescaling-noise}
442
+ \end{align}
443
+ Since $\sum_t a_t\le1$, it follows that
444
+ \[
445
+ \E\left|\overline M_P-\sum_t a_t\right|
446
+ \le\sum_t\frac{a_t}{p_t}\E|p'_t-p_t|
447
+ \le\frac{\gamma+\sqrt{g(1+\gamma)}}{p_0}.
448
+ \]
449
+ Use the identity $y(U\cap F_j)+\sum_t a_t=1$, the triangle inequality,
450
+ and the second-moment bounds in
451
+ Equations~\ref{eq:prep-outside-noise}--\ref{eq:prep-conditional-noise}.
452
+ The expected shortfall is at most
453
+ \begin{equation}\label{eq:prep-shortfall}
454
+ \E(1-M_U-M_P)_+\le H,
455
+ \qquad
456
+ H:=\sqrt g+\sqrt{g/p_0}
457
+ +\frac{\gamma+\sqrt{g(1+\gamma)}}{p_0}.
458
+ \end{equation}
459
+ In particular no independence between outside counts and rescaled
460
+ bundle masses is being assumed.
461
+
462
+ Trim any surplus mass on $F_j$, which cannot increase its cost. To
463
+ fill a remaining shortfall, there is always one unit of available
464
+ opening within distance
465
+ \[
466
+ QV_j,\qquad Q:=M+(1+\delta)T_1,
467
+ \]
468
+ from $j$. Indeed, if $c_s=0$, there are no activations at $s$ and $P_s$
469
+ has exactly one unit, all at distance at most
470
+ $D+R_s\le(M+T_1)V_j$. If $c_s>0$, use $P_s$ and the bundle $P_t$ of a
471
+ nearest other representative. They are disjoint and each has at
472
+ least half a unit. Their supply lies within distance
473
+ $D+(1+\delta)L_s\le QV_j$.
474
+ This supply can fill the shortfall even if some of it is already used:
475
+ if the current assignment has mass $1-q$, a ball containing at least
476
+ one opening unit contains at least $q$ unused units. Allocate those
477
+ units to finish the assignment. By Equation~\ref{eq:prep-shortfall},
478
+ the unconditional expected nearest-unit cost is at most
479
+ $B_{\mathrm{near}}V_j$, where
480
+ \begin{equation}\label{eq:prep-near-factor}
481
+ B_{\mathrm{near}}:=p_0^{-1}+QH.
482
+ \end{equation}
483
+
484
+ \paragraph{Choosing parameters and enforcing the budget.}
485
+ Equations~\ref{eq:prep-far-factor} and~\ref{eq:prep-near-factor} give
486
+ explicit bounds that approach one in the stated order of parameter
487
+ choices. More precisely, first choose $\delta$ small to make the
488
+ limiting value of $\kappa$ close to one. Next choose $M$ large so that
489
+ $p_0^{-1}$ is close to one, and then choose $T_1$ large so that $\alpha$
490
+ and $\beta$ are small. With these constants fixed, choose $\gamma$
491
+ small enough to control both the last term of $B_{\mathrm{far}}$ and
492
+ the term $Q\gamma/p_0$ in $B_{\mathrm{near}}$. Finally choose $g$ small
493
+ enough to control all square-root terms and $\rho$ in
494
+ Equation~\ref{eq:prep-budget-probability}. All constants may be
495
+ rational, and all sufficiently small $g=1/\Delta$ with even $\Delta$
496
+ satisfy the resulting strict bounds. In particular, arrange
497
+ \[
498
+ \rho<\tfrac12,\qquad
499
+ \frac{\max\{B_{\mathrm{far}},B_{\mathrm{near}}\}}{1-\rho}
500
+ \le1+\eta.
501
+ \]
502
+
503
+ Reject a star-rounding outcome outside $\mathcal G$ and repeat.
504
+ For the purpose of the preceding unconditional analysis, the subsequent
505
+ bundle rounding can be imagined on every outcome. Let
506
+ $\widetilde V_j$ denote the resulting nearest-unit cost. Its
507
+ nonnegativity, rather than any independence from $\mathcal G$, gives
508
+ \begin{equation}\label{eq:prep-cost-final}
509
+ \E[\widetilde V_j\mid\mathcal G]
510
+ \le\frac{\E\widetilde V_j}{\Prob(\mathcal G)}
511
+ \le(1+\eta)V_j.
512
+ \end{equation}
513
+ The already established supply and opening bounds hold on every
514
+ accepted outcome.
515
+
516
+ The split representation, star list, and number of pair updates are
517
+ polynomial in the input size. Pair updates and subset choices use
518
+ rational probabilities and rational linear operations. Their
519
+ encodings have polynomial bit length: each weighted update introduces
520
+ only ratios of integer weights bounded by $|\mathcal S|$, and there
521
+ are polynomially many updates; the subsequent rescalings divide by
522
+ the rational masses $p_s$. Exact rational sampling has expected
523
+ polynomial running time. The acceptance probability is at least
524
+ one half, so rejection multiplies the expected running time by at
525
+ most two. This proves the theorem.
526
+ \end{proof}
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/build/sections/rounding.tex ADDED
@@ -0,0 +1,871 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Tapered iterative rounding}\label{sec:rounding}
2
+
3
+ This section rounds a sufficiently fine grid solution. The graph used for
4
+ rounding gives every active copy one unit of possible incoming erasers.
5
+ Its distance-dependent taper makes the opening that accompanies an erasure
6
+ comparable to the client's surviving candidates. A potential that retains
7
+ some cheap candidates after an opening converts this comparison into an
8
+ application of Theorem~\ref{thm:finite-inequality}.
9
+
10
+ \begin{theorem}[Rounding a grid solution]\label{thm:grid-rounding}
11
+ For every fixed $\tau>0$ and all sufficiently large constant integers
12
+ $\Delta$, put $g=1/\Delta$. Suppose a finite rational metric instance has openings
13
+ $\widetilde y_i\in[0,1]\cap g\mathbb Z$ of total mass $M\ge1$.
14
+ For a client $j$, let $V_{j,0}$ be the cost of its nearest unit of this mass.
15
+ There is a constant $C=C(\tau,\Delta)$ and a randomized algorithm of
16
+ expected polynomial running time that outputs a set $O$ of facilities with
17
+ \[
18
+ |O|\le M+C,
19
+ \qquad
20
+ \E d(j,O)\le(1+2/e+\tau)V_{j,0}\quad\text{for every client }j.
21
+ \]
22
+ All parameters and the additive constant are independent of the instance.
23
+ In particular, an initial mass at most $k+c_0$, for a fixed constant
24
+ $c_0$, gives at most $k+c_0+C$ facilities.
25
+ The deterministic implementation of the resulting total-cost guarantee
26
+ is given in Section~\ref{sec:derandomization}.
27
+ \end{theorem}
28
+
29
+ We prove the theorem using the functions $A,P,B,m$ defined in the preceding
30
+ section. Thus $B(x)=2P(x)=A'(x)$ and
31
+ $m(x)=A(x)-1-xB(x)$. We use, in particular,
32
+ \begin{equation}\label{eq:rnd-function-identities}
33
+ \begin{gathered}
34
+ 0<B(x)\le1,\qquad B(x)\ge2P(1)>0,\qquad m(x)\ge0,\\
35
+ (1+x)A(x)+xB(x)-1=3x\qquad(0\le x\le1).
36
+ \end{gathered}
37
+ \end{equation}
38
+ The identities and derivative bounds used below follow directly from
39
+ the defining integrals. Constants implicit in $O_\Delta(\cdot)$ may
40
+ depend on $\Delta$, but not on the instance, the round, or the subsequent
41
+ heavy-source threshold.
42
+
43
+ \subsection{The graph and the physical process}
44
+
45
+ The source-opening and neighbor-erasure operation follows the framework
46
+ of Byrka et al.~\cite[Definitions~3.2 and~5.1]{ByrkaEtAl2026}.
47
+ We specify the graph, taper, and batches here because their precise
48
+ properties will be used in the sub-two drift analysis.
49
+
50
+ Represent each opening by active copies of mass $g$, grouped by facility.
51
+ Each group has at most $\Delta$ active copies. Co-located facilities
52
+ introduced by earlier splitting may remain distinct groups throughout
53
+ the process; they can be merged in the output. A group always means one
54
+ such labeled facility group, rather than an entire zero-distance class.
55
+ An integral group has exactly $\Delta$ copies.
56
+
57
+ Fix a small time step $\ell>0$ and a large time horizon $\Lambda$.
58
+ There are $T=\lceil\Lambda/\ell\rceil$ rounds. At the start of round
59
+ $r\in\{0,\ldots,T-1\}$ let $\xi=r\ell$ and $x=e^{-\xi}$.
60
+ For that round choose a fixed rational number $\widehat P$ satisfying
61
+ \begin{equation}\label{eq:rnd-taper-approximation}
62
+ 0<\widehat P\le\tfrac12,
63
+ \qquad |\widehat P-P(x)|\le\zeta,
64
+ \qquad 0<\zeta<\tfrac14.
65
+ \end{equation}
66
+ The finitely many rational approximations may be fixed in advance.
67
+ The analytic value $x$ is used only in the analysis.
68
+
69
+ For each active target copy $i$, independently of the other targets
70
+ conditional on the current state, choose a set $\mathcal H_i$ of exactly
71
+ $\Delta$ active source copies. If the colocated active mass is below one,
72
+ choose $N_i>0$ minimally so that
73
+ \begin{equation}\label{eq:rnd-edge-marginals}
74
+ q_{hi}=\min\left\{1,\frac{(1-d(i,h)/N_i)_+}{\widehat P}\right\},
75
+ \qquad \sum_h gq_{hi}=1,
76
+ \end{equation}
77
+ and give $\mathcal H_i$ these marginals. Such a radius exists: the sum
78
+ is continuous and nondecreasing in the positive radius, starts below
79
+ one, and reaches the total active mass at a finite radius. This last
80
+ observation also handles total active mass exactly one. The equation
81
+ is piecewise linear in $1/N_i$. Fixed-sum rounding realizes the
82
+ marginals since their unscaled sum is the integer $\Delta$.
83
+
84
+ If the colocated active mass is already at least one, set $N_i=0$ and
85
+ choose $\Delta$ colocated copies, including every active copy in the
86
+ target's own group. Any fixed such choice suffices in this case; denote
87
+ its marginals by $q_{hi}$ as well. In either case every own-group copy
88
+ belongs to $\mathcal H_i$ with certainty, and
89
+ \begin{equation}\label{eq:rnd-taper-comparison}
90
+ \begin{aligned}
91
+ N_i(1-\widehat Pq_{hi})&\le d(i,h)&&\text{if }q_{hi}<1,\\
92
+ d(i,h)&\le N_i(1-\widehat Pq_{hi})&&\text{if }q_{hi}>0.
93
+ \end{aligned}
94
+ \end{equation}
95
+ For $N_i>0$ these statements follow from the three cases of the clipped
96
+ linear formula; for $N_i=0$ all sources of positive marginal are
97
+ colocated. Define the out-set of source $h$ by
98
+ \[
99
+ E_h=\{i:h\in\mathcal H_i\}.
100
+ \]
101
+ A full update at $h$ erases $E_h$ and opens the facility of $h$.
102
+
103
+ We use balanced and biased unbalanced batches, with forced openings for
104
+ large updates, as in the approach of Byrka et
105
+ al.~\cite[Algorithms~4--5 and Section~5.4]{ByrkaEtAl2026}.
106
+ The exact batch and chunk rules below are part of our construction.
107
+ To implement many updates while controlling the total opening mass, put
108
+ \[
109
+ u_h=1-g|E_h|,
110
+ \qquad
111
+ \mathcal Z=\{h:u_h=0\},\quad
112
+ \mathcal P=\{h:u_h>0\},\quad
113
+ \mathcal N=\{h:u_h<0\}.
114
+ \]
115
+ Every target has $\Delta$ incoming sources, so $\sum_hu_h=0$. Write
116
+ \begin{equation}\label{eq:rnd-balance-size}
117
+ A_* =\sum_{h\in\mathcal P}u_h
118
+ =\sum_{h\in\mathcal N}|u_h|,
119
+ \qquad
120
+ |\mathcal P\cup\mathcal N|\le 2A_*/g.
121
+ \end{equation}
122
+ The last inequality uses that each nonzero $u_h$ is a nonzero multiple
123
+ of $g$. Choose a further small constant $b_*>0$, to be fixed last, and put
124
+ \[
125
+ B_* =\max\{1,b_*A_*\}.
126
+ \]
127
+ A source is \emph{heavy} if $g|E_h|>B_*$. Force open the facilities of
128
+ all heavy sources, whether or not any random update is triggered.
129
+
130
+ All random choices and erasure sets in a round refer to its pre-round
131
+ graph and active copies. Set $p_*=2\ell g$, and fix a small bias
132
+ $0<\phi\le1$. Flip an independent fair coin to choose one of the following
133
+ two types of round.
134
+ \begin{enumerate}
135
+ \item In a balanced round, propose each $h\in\mathcal Z$ independently
136
+ with probability $p_*$. Select a proposed source only if no other
137
+ proposed source has an out-set intersecting its out-set.
138
+ \item In an unbalanced round, select sources of $\mathcal P$
139
+ independently with probability $p_*$, and nonheavy sources of
140
+ $\mathcal N$ independently with probability $p_*(1+\phi)$.
141
+ For each heavy source, partition its out-set into chunks of mass at
142
+ most $B_*+1$ and trigger each chunk independently with probability
143
+ $p_*(1+\phi)$. A triggered chunk erases just that chunk; its source
144
+ facility is already included among the forced openings.
145
+ \end{enumerate}
146
+ All probabilities are at most one for the parameter choices below.
147
+ Take the union of the selected full out-sets and triggered chunks and
148
+ erase it. Then reset each forced or selected facility to $\Delta$
149
+ active copies. Copies removed by either erasure or reset are distinct
150
+ from the regenerated copies.
151
+
152
+ Two invariants are useful. First, an integral target group's own
153
+ $\Delta$ copies exhaust each of its incoming sets. Therefore an
154
+ erasure of an integral group is caused by one of its own sources; that
155
+ source either is selected or is heavy. The group is reset in either
156
+ case. Thus integral facilities persist, including when other facilities
157
+ are colocated with them. Second, every erasure has an associated
158
+ selected or forced opening. Hence total active mass always stays at
159
+ least one. The construction of the next round's graph is consequently
160
+ well defined.
161
+
162
+ \subsection{The opening-count bound}
163
+
164
+ We first bound the number of facilities independently of connection cost.
165
+ The next lemma controls the total active mass with high probability;
166
+ completion will later turn that mass bound into a facility-count bound.
167
+
168
+ \begin{lemma}[Constant additive count]\label{lem:rnd-count}
169
+ Fix $g,\phi,\ell,T$ as above, with $\ell$ sufficiently small as a
170
+ function of $\Delta$ and $\phi$. For every fixed $\eta>0$, one can
171
+ choose $b_*>0$ and a constant $C$ such that the final active mass is at
172
+ most $M+C$ with probability at least $1-\eta$. The bound holds
173
+ uniformly over all starting states of total mass $M$.
174
+ \end{lemma}
175
+
176
+ \begin{proof}
177
+ Condition on the entire pre-round state and its realized graph.
178
+ Write $A=A_*$, $B=B_*$, $p=p_*$, and $m_h=g|E_h|$ for this proof.
179
+ If $n$ is the number of active copies, then $\sum_hm_h=n$.
180
+ Each source in the zero class has $m_h=1$, so removing that class gives
181
+ \[
182
+ \sum_{h\in\mathcal P\cup\mathcal N}m_h
183
+ =|\mathcal P\cup\mathcal N|.
184
+ \]
185
+ Every heavy source lies in $\mathcal N$ because $B\ge1$. If $H$ is
186
+ their number, then
187
+ \begin{equation}\label{eq:rnd-heavy-count}
188
+ H\le\frac{|\mathcal P\cup\mathcal N|}{B}
189
+ \le\frac{2A}{g\max\{1,b_*A\}}
190
+ \le\frac{2}{gb_*}.
191
+ \end{equation}
192
+ Thus forced resets add at most a constant mass. If $A=0$, there are
193
+ no heavy sources and the same conclusions hold directly.
194
+
195
+ In a balanced round, the selected erasure sets are disjoint and each
196
+ has mass one. Opening one facility for each selected source adds at
197
+ most one unit per set, so there is no mass increase except the forced
198
+ allowance.
199
+
200
+ For an unbalanced round index the ordinary selections and heavy
201
+ chunks by actions $e$. Let $I_e$ be the trigger indicator, $S_e$ its
202
+ erased set, $m_e=g|S_e|$, and $a_e=1$ for an ordinary selection or $0$
203
+ for a chunk. Resetting facilities adds at most one unit per ordinary
204
+ selection in addition to the forced allowance. More explicitly, the
205
+ change in active mass is at most
206
+ \[
207
+ H+\sum_e a_e I_e
208
+ -g\left|\bigcup_{e:I_e=1}S_e\right|.
209
+ \]
210
+ The union is a set of pre-round copy identities. A reset may remove
211
+ additional old copies outside this union, which only decreases the
212
+ change. Counting a selected or forced group more than once likewise
213
+ only enlarges the upper bound. Truncated inclusion--exclusion bounds
214
+ the erased union from below. Consequently the mass increase, apart
215
+ from forcing, is at most
216
+ \begin{equation}\label{eq:rnd-count-statistic}
217
+ Z_* =\sum_e I_e(a_e-m_e)
218
+ +\sum_{e<f}g|S_e\cap S_f|I_eI_f.
219
+ \end{equation}
220
+ This remains an upper bound when several selected copies have the
221
+ same facility or when a selected facility was also forced.
222
+
223
+ Chunking preserves total erasure mass. There are
224
+ $|\mathcal P\cup\mathcal N|-H$ ordinary actions, and hence
225
+ \begin{equation}\label{eq:rnd-action-total}
226
+ \sum_e(m_e+a_e)
227
+ =2|\mathcal P\cup\mathcal N|-H\le4A/g.
228
+ \end{equation}
229
+ The expectation of the linear part of \eqref{eq:rnd-count-statistic}
230
+ is exactly
231
+ \[
232
+ pA-p(1+\phi)A-p(1+\phi)H\le-p\phi A.
233
+ \]
234
+ The last term pays for the absence of a new opening in a chunk action.
235
+ Each target belongs to at most $\Delta$ action sets, even after
236
+ chunking. Therefore
237
+ \[
238
+ \sum_{e<f}g|S_e\cap S_f|
239
+ \le\frac{\Delta-1}{2}\sum_em_e.
240
+ \]
241
+ Independence of the indicators bounds the overlap expectation by
242
+ $O(p^2\Delta A/g)$. Since $p=2\ell g$, taking $\ell$ small enough
243
+ relative to $\phi$ and $\Delta$ gives
244
+ \begin{equation}\label{eq:rnd-count-mean}
245
+ \E Z_*\le-p\phi A/2.
246
+ \end{equation}
247
+
248
+ Flipping coordinate $I_e$ changes $Z_*$ in absolute value by at most
249
+ $a_e+\Delta m_e$. The Efron--Stein independent-coordinate variance inequality
250
+ \cite[Section~2.2, Proposition~1]{BBLM2005}, the bound
251
+ $a_e+m_e\le B+2$, and \eqref{eq:rnd-action-total} give
252
+ \begin{equation}\label{eq:rnd-count-variance}
253
+ \Var Z_*
254
+ \le O(p\Delta^2)\sum_e(a_e+m_e)^2
255
+ \le O(p\Delta^2)(B+2)A/g.
256
+ \end{equation}
257
+ If $A>1/b_*$, then $B=b_*A>1$. Combining
258
+ \eqref{eq:rnd-count-mean} and \eqref{eq:rnd-count-variance} yields
259
+ \begin{equation}\label{eq:rnd-count-failure}
260
+ \Prob(Z_*>0)
261
+ \le O\!\left(\frac{\Delta^2b_*}{p\phi^2g}\right).
262
+ \end{equation}
263
+ If instead $A\le1/b_*$, there are at most $2/(gb_*)$ ordinary
264
+ sources in the nonzero classes. The actual positive mass change is
265
+ then bounded deterministically by this constant plus the forced
266
+ allowance; a deterministic bound on the quadratic statistic is
267
+ unnecessary.
268
+
269
+ Choose $b_*$ sufficiently small that the union bound for
270
+ \eqref{eq:rnd-count-failure} over the $T$ rounds is at most $\eta$.
271
+ On the complementary event the total increase is at most, for example,
272
+ $4T/(gb_*)$. This proves the lemma with a constant $C$.
273
+ The proof was conditional on every state and graph, so the same union
274
+ bound applies to the adaptive sequence of rounds.
275
+ \end{proof}
276
+
277
+ For later use, the mean and variance of $Z_*$ depend only on indicator
278
+ moments through degree four, since $Z_*$ is a quadratic polynomial.
279
+ The probability bounds for balanced selections below need only
280
+ first and second moments of their proposal indicators. These are
281
+ the moment requirements used in Section~\ref{sec:derandomization}.
282
+
283
+ \subsection{A persistent backup and final completion}
284
+
285
+ We next establish a persistent bound on each client's eventual
286
+ connection distance, including trajectories on which none of its assigned
287
+ copies opens. This is the backup-and-completion role in iterative
288
+ rounding~\cite[Section~3.3 and Lemmas~6.3 and~6.5]{ByrkaEtAl2026};
289
+ the following argument proves the bound for our tapered graph and reset
290
+ rule.
291
+
292
+ Fix a client for the remainder of the analysis. Let $S_0$ be the
293
+ $\Delta$ copies in its initial nearest unit, chosen using any fixed
294
+ tie-breaking rule. Write $d_i$ for its distance to copy $i$,
295
+ \[
296
+ V_0=\sum_{i\in S_0}gd_i,
297
+ \qquad R=\max_{i\in S_0}d_i.
298
+ \]
299
+ In particular $R\le\Delta V_0$.
300
+
301
+ \begin{lemma}[Backup and completion]\label{lem:rnd-completion}
302
+ Once a copy of $S_0$ is physically removed, an integral facility within
303
+ distance $5R$ of the client exists and persists to the end.
304
+ At the end of the process one can retain all integral facilities and
305
+ open further facilities, using no more than the total final active
306
+ mass, so that every client is connected within its own distance $5R$.
307
+ \end{lemma}
308
+
309
+ \begin{proof}
310
+ Consider the round of the first physical removal from $S_0$. Just
311
+ before that round all of $S_0$ is still active. For $i,t\in S_0$,
312
+ $d(i,t)\le d_i+d_t\le2R$. At radius $2R/(1-\widehat P)$, the
313
+ $\Delta$ copies of $S_0$ all have incoming marginal one for target
314
+ $i$. Minimality of the taper radius gives
315
+ \[
316
+ N_i\le2R/(1-\widehat P)\le4R.
317
+ \]
318
+ If $R=0$, the zero-radius rule gives the same conclusion directly.
319
+ An erasing source $h$ has $d(i,h)\le N_i$ by
320
+ \eqref{eq:rnd-taper-comparison}, and hence $d_h\le5R$.
321
+ Its facility is either selected or forced open. A removal by reset
322
+ of $i$'s own group instead opens a facility within $R$.
323
+ The persistence invariant proves the first assertion.
324
+
325
+ At the end, consider the clients not already served within $5R$ by
326
+ an integral facility. The first assertion implies that every such
327
+ client still has all its original $S_0$ copies. Its radius-$R$
328
+ neighborhood of active copies therefore has mass at least one.
329
+ That neighborhood contains no integral group, since such a group
330
+ would itself provide the required connection.
331
+
332
+ Process these neighborhoods in nondecreasing order of their radii.
333
+ Accept a neighborhood if it is disjoint from all previously accepted
334
+ ones and open any facility in each accepted neighborhood. These
335
+ disjoint neighborhoods each contain at least one unit of mass and
336
+ contain no integral group. Their openings, together with the retained
337
+ integral groups, therefore fit within the final active mass.
338
+ If a radius-$R$ neighborhood was skipped, it meets an accepted
339
+ radius-$R'$ neighborhood with $R'\le R$. Through an intersection
340
+ point, the distance to the accepted neighborhood's chosen facility
341
+ is at most $R+2R'\le3R$. This proves the asserted $5R$ bound for
342
+ every client, also when some radii are zero.
343
+ \end{proof}
344
+
345
+ At any intermediate time define $b$ to be the distance from the fixed
346
+ client to its nearest integral facility, capped at $5R$; when no
347
+ integral facility exists use $b=5R$. By persistence and
348
+ Lemma~\ref{lem:rnd-completion}, the eventual completed solution has
349
+ connection distance at most $b$ at every time on the trajectory.
350
+ The cap need not already be attained by an open facility. It is a
351
+ valid bound on the eventual connection because completion supplies
352
+ $5R$ on every trajectory. The quantity $b$ never increases.
353
+
354
+ \subsection{The potential and its single-action bounds}
355
+
356
+ For analysis only, track an alive set $S\subseteq S_0$ of original
357
+ copies. A physically removed copy leaves $S$ permanently, even when
358
+ its facility is reset with regenerated copies. We also permit the
359
+ additional discards specified below. Put
360
+ \[
361
+ y=g|S|,\qquad V=\sum_{i\in S}gd_i.
362
+ \]
363
+ At elapsed time $\xi$, with $x=e^{-\xi}$, define
364
+ \begin{equation}\label{eq:rnd-potential}
365
+ f=aV+(1-y)b,
366
+ \qquad
367
+ a=A(x)+B(x)(y-x)=1+m(x)+B(x)y.
368
+ \end{equation}
369
+ The coefficient $a$ is the value at $y$ of the tangent line to the
370
+ concave function $A$ at $x$; $x$ is a deterministic clock, while $y$
371
+ is the realized alive mass. Its affine dependence on $y$ makes the
372
+ erasure correction quadratic in removed mass and cost, so the graph
373
+ average of the ideal bound below requires only first and second edge
374
+ moments.
375
+ In particular $a\ge1$. The initial potential is
376
+ \begin{equation}\label{eq:rnd-initial-potential}
377
+ f_0=A(1)V_0=(1+2/e)V_0.
378
+ \end{equation}
379
+ If $C_j$ denotes the actual connection distance in the completed
380
+ output, the preceding cap property gives
381
+ \begin{equation}\label{eq:rnd-terminal-correction}
382
+ C_j-f_T\le y_Tb_T-a_TV_T\le5Ry_T.
383
+ \end{equation}
384
+ The potential and every single-action bound below are $O(R)$ uniformly
385
+ over time: $V\le R$, $0\le y\le1$, $b\le5R$, and $a$ is bounded.
386
+
387
+ We first freeze time and the graph. Write $B=B(x)$ and
388
+ $b_h=\min\{b,d_h\}$. For a source $h\notin S$, let
389
+ \[
390
+ \delta_h=g|E_h\cap S|,
391
+ \qquad Y_h=\sum_{i\in E_h\cap S}gd_i.
392
+ \]
393
+ If only this full source update affects $S$, its removal changes the
394
+ coefficient to $a-B\delta_h$ and makes the new cap at most $b_h$.
395
+ Its potential change is consequently at most
396
+ \begin{align*}
397
+ &(a-B\delta_h)(V-Y_h)+(1-y+\delta_h)b_h-f\\
398
+ &\quad=\delta_hb_h-aY_h-B\delta_h(V-Y_h)
399
+ +(1-y)(b_h-b)\\
400
+ &\quad\le\delta_hb_h-aY_h-B\delta_h(V-Y_h).
401
+ \end{align*}
402
+ The same statement holds when $h$ is not alive but its group contains
403
+ alive copies: all those copies belong to $E_h$ by the own-group edges,
404
+ so its reset creates no unaccounted removal.
405
+
406
+ If an alive source $h\in S$ opens, retain among the physical survivors
407
+ only copies satisfying $ad_i<d_h$. If their mass and cost are $y',V'$,
408
+ their new coefficient is at most $a$ and their new cap is at most
409
+ $d_h$. Therefore
410
+ \[
411
+ f'\le aV'+(1-y')d_h
412
+ =d_h-\sum_{\substack{i\in S\\h\notin\mathcal H_i}}
413
+ g(d_h-ad_i)_+.
414
+ \]
415
+ Copies satisfying equality can be discarded without changing this
416
+ bound. Figure~\ref{fig:survivors} separates physical erasure from these
417
+ additional analysis discards. This continuation after an opening
418
+ supplies the subtraction that will enter
419
+ Theorem~\ref{thm:finite-inequality}.
420
+
421
+ \input{figures/survivors}
422
+
423
+ The ideal first-order bound, assigning rate $g$ to each full source
424
+ update, is thus
425
+ \begin{equation}\label{eq:rnd-ideal-generator}
426
+ \begin{aligned}
427
+ \mathcal B={}&
428
+ \sum_{h\in S}g\left[
429
+ d_h-\sum_{\substack{i\in S\\h\notin\mathcal H_i}}
430
+ g(d_h-ad_i)_+-f\right]\\
431
+ &+\sum_{h\notin S}g\left[
432
+ \delta_hb_h-aY_h-B\delta_h(V-Y_h)\right].
433
+ \end{aligned}
434
+ \end{equation}
435
+ At a fixed alive set and cap, the time derivative is
436
+ \begin{equation}\label{eq:rnd-time-derivative}
437
+ \dot f=-x(y-x)B'(x)V.
438
+ \end{equation}
439
+ Indeed the derivative of $A(x)+B(x)(y-x)$ with respect to $x$ is
440
+ $B'(x)(y-x)$.
441
+
442
+ \subsection{From the physical batch to the ideal bound}
443
+
444
+ For the actual analysis update, first account for forced openings by
445
+ removing from $S$ all copies whose groups are forced and updating the
446
+ cap. Then apply the round's erasures and resets. If a source that
447
+ was alive after force removals but before these erasures was selected,
448
+ choose one such source $h$ and discard every remaining copy with
449
+ $ad_i\ge d_h$, using the pre-round value of $a$. This is purely an
450
+ analysis rule and need not be computed by the algorithm.
451
+
452
+ \begin{lemma}[Conditional batch drift]\label{lem:rnd-batch}
453
+ For every pre-round history and every realized graph, the physical
454
+ round, the above alive-set update, and the time advance satisfy
455
+ \begin{equation}\label{eq:rnd-batch-drift}
456
+ \E[f_{r+1}-f_r\mid\text{history, graph}]
457
+ \le\ell(\dot f+\mathcal B)
458
+ +O_\Delta\bigl((\phi+\ell)\ell R\bigr).
459
+ \end{equation}
460
+ Here $\mathcal B$ is computed from that graph and the original
461
+ pre-round alive set. The constants and the required upper bound on
462
+ $\ell$ are uniform in $b_*$.
463
+ \end{lemma}
464
+
465
+ \begin{proof}
466
+ First suppose no group containing an alive copy is forced. Call an
467
+ action relevant if its ordinary source is in $S$, or its ordinary
468
+ out-set or heavy chunk meets $S$. There are at most
469
+ $\Delta^2+\Delta$ relevant actions: each of at most $\Delta$ alive
470
+ targets has $\Delta$ incoming sources. Own-group edges ensure that
471
+ this list also includes every ordinary reset that can affect $S$.
472
+
473
+ A balanced source has an out-set of exactly $\Delta$ copies. Every
474
+ one of those copies belongs to at most $\Delta$ source out-sets, so
475
+ the number $c_h$ of potentially conflicting balanced proposals is at
476
+ most $\Delta^2$. Including the type coin, its selection marginal is
477
+ \[
478
+ \tfrac12p_*(1-p_*)^{c_h}
479
+ =\ell g\bigl(1+O_\Delta(\ell)\bigr).
480
+ \]
481
+ An unbalanced ordinary or chunk action has marginal $\ell g$ or
482
+ $(1+\phi)\ell g$. Any two distinct actions have joint probability
483
+ $O(\ell^2g^2)$; actions of opposite types have joint probability zero.
484
+ These estimates do not assert independence of balanced selections
485
+ after conflict filtering.
486
+
487
+ If no relevant action occurs, only the cap can improve, so the
488
+ frozen-time potential cannot increase. If exactly one relevant
489
+ ordinary action occurs, its change is bounded by the appropriate
490
+ single-source expression in \eqref{eq:rnd-ideal-generator}.
491
+ Unrelated selections or forced openings can only lower its cap and
492
+ do not invalidate that upper bound. The probability of two or more
493
+ relevant actions is $O_\Delta(\ell^2)$, and all possible potentials
494
+ and individual bounds have magnitude $O(R)$. Replacing isolated-action
495
+ probabilities by marginals and their marginals by $\ell g$ therefore
496
+ costs $O_\Delta((\phi+\ell)\ell R)$.
497
+
498
+ For a heavy source outside $S$, its forced facility makes the cap at
499
+ most $b_h$ even when only one of its chunks triggers. Force accounting
500
+ can be done before erasure accounting because no forced group in the
501
+ present case meets $S$; it only improves the cap. Write
502
+ $\delta_c,Y_c$ for the alive mass and cost removed by chunk $c$ of
503
+ this source, and $\delta=\sum_c\delta_c$, $Y=\sum_cY_c$. Its summed
504
+ single-chunk bounds satisfy
505
+ \begin{align*}
506
+ \sum_c[\delta_cb_h-aY_c-B\delta_c(V-Y_c)]
507
+ &=\delta b_h-aY-B\delta V+B\sum_c\delta_cY_c\\
508
+ &\le\delta b_h-aY-B\delta(V-Y).
509
+ \end{align*}
510
+ All cross terms omitted in the last step are nonnegative. Consequently
511
+ the chunk bounds are dominated by the full-source term used in
512
+ $\mathcal B$.
513
+
514
+ The functions in the potential have uniformly bounded derivatives.
515
+ The chance that a relevant action changes $S$ is $O_\Delta(\ell)$;
516
+ changes of the cap alone do not affect \eqref{eq:rnd-time-derivative}.
517
+ Advancing time thus adds at most
518
+ $\ell\dot f+O_\Delta(\ell^2R)$. This proves the lemma when no alive
519
+ group is forced.
520
+
521
+ Now suppose that forcing does remove alive copies. Let their total
522
+ mass and cost be $\delta\ge g$ and $Y$, and let $b'\le b$ be the
523
+ cap after force accounting. Every removed copy is in an opened
524
+ facility, so $Y\ge\delta b'$. At frozen time, the resulting decrease
525
+ is at least
526
+ \begin{align}
527
+ f-f'
528
+ &\ge(a-1)Y+B\delta(V-Y)+(1-y)(b-b')\notag\\
529
+ &\ge BgV+(1-y)(b-b').\label{eq:rnd-force-savings}
530
+ \end{align}
531
+ For the second line, use $a-1=m+By$, $m\ge0$, and
532
+ $y\ge\delta\ge g$. At least one removed alive copy has distance
533
+ at most $V/g$, so $b'\le V/g$. With
534
+ \[
535
+ Q=V+(1-y)b,\qquad D=(1-y)(b-b'),
536
+ \]
537
+ we obtain
538
+ \[
539
+ \begin{gathered}
540
+ Q\le(1+1/g)V+D,\qquad BgV+D\ge c_\Delta Q,\\
541
+ c_\Delta=\min\left\{1,\frac{2P(1)g}{1+1/g}\right\}>0.
542
+ \end{gathered}
543
+ \]
544
+ Thus forcing supplies a fixed fraction of $Q$ as free savings.
545
+
546
+ After force accounting, the remaining alive cost is at most $V$ and
547
+ the cap is at most $V/g$. Any further frozen-time increase has
548
+ magnitude $O_\Delta(V)$, and a change to the alive set still has
549
+ probability $O_\Delta(\ell)$. If the alive set does not change, the
550
+ cap only improves. Subsequent actions and time advance therefore
551
+ have expected increase at most $O_\Delta(\ell Q)$.
552
+
553
+ For comparison with the pre-force ideal expression, we also have
554
+ \begin{equation}\label{eq:rnd-force-generator-size}
555
+ |\dot f|+|\mathcal B|\le O_\Delta(Q).
556
+ \end{equation}
557
+ For inside sources, $d_h\le V/g$. If $y<1$, the grid gives
558
+ $1-y\ge g$, so an external cap charge is bounded using $b\le Q/g$.
559
+ If $y=1$, the alive set itself is a full unit; its maximum distance
560
+ is at most $V/g$. The radius argument from
561
+ Lemma~\ref{lem:rnd-completion} then bounds any source erasing an alive
562
+ copy within $5V/g$ of the client. Only $O_\Delta(1)$ sources have
563
+ nonzero contributions. These observations prove
564
+ \eqref{eq:rnd-force-generator-size}.
565
+
566
+ Choose $\ell$ sufficiently small in terms of these constants and
567
+ $c_\Delta$. The savings in \eqref{eq:rnd-force-savings} absorb both
568
+ the subsequent expected increase and the possible negative quantity
569
+ $\ell(\dot f+\mathcal B)$. This proves
570
+ \eqref{eq:rnd-batch-drift} also in the forced case, without an
571
+ additional error term. If $Q=0$, all the quantities in this
572
+ comparison vanish, so no division by $Q$ is needed. More explicitly,
573
+ if $V=0$ then $b'=0$, and the force savings remove $(1-y)b$; when
574
+ also $y=1$, relevant source distances and all generator terms are
575
+ zero. The argument is uniform in the later choice of $b_*$.
576
+ \end{proof}
577
+
578
+ The order of conditioning in Lemma~\ref{lem:rnd-batch} is essential.
579
+ Whether a group is forced depends on the graph. We have proved the
580
+ drift comparison for \emph{every} realized graph, in both force cases;
581
+ we will now average that comparison over the original graph law,
582
+ without conditioning the law on a forcing event.
583
+
584
+ \subsection{Averaging the graph and applying the finite inequality}
585
+
586
+ The physical batch has now been compared with the ideal generator for
587
+ every realized graph. We average that generator using edge marginals and
588
+ cross-target second moments, then verify the hypotheses of the abstract
589
+ finite comparison inequality. The resulting bound is the cost estimate
590
+ that will be summed over rounds.
591
+
592
+ \begin{lemma}[Averaged ideal drift]\label{lem:rnd-average}
593
+ Conditional on the pre-round history, the ideal expression satisfies
594
+ \begin{equation}\label{eq:rnd-average-drift}
595
+ \dot f+\E_{\mathrm{graph}}\mathcal B
596
+ \le BgV+12\zeta V.
597
+ \end{equation}
598
+ \end{lemma}
599
+
600
+ \begin{proof}
601
+ The pre-round quantities $S,y,V,b,x$ are fixed throughout this proof.
602
+ Define
603
+ \begin{equation}\label{eq:rnd-graph-statistics}
604
+ \begin{aligned}
605
+ w_i&=\sum_{t\in S}gq_{ti},\\
606
+ K_{it}&=\sum_{h\notin S}gq_{hi}q_{ht},\\
607
+ s_i&=\frac{\sum_{h\notin S}gq_{hi}^2}{1-w_i}
608
+ \quad\text{if }w_i<1,
609
+ \qquad s_i=0\quad\text{if }w_i=1.
610
+ \end{aligned}
611
+ \end{equation}
612
+ We have $0\le w_i\le y\le1$ and $0\le s_i\le1$.
613
+ The inequality $2uv\le u^2+v^2$ gives
614
+ \begin{equation}\label{eq:rnd-kernel-bound}
615
+ K_{it}\le\tfrac12\bigl[s_i(1-w_i)+s_t(1-w_t)\bigr].
616
+ \end{equation}
617
+ No symmetry of the directed marginals $q_{hi}$ is assumed.
618
+
619
+ To average the positive quadratic erasure term, put
620
+ $X_{hi}=\ind_{\{h\in\mathcal H_i\}}$. Choices for distinct targets
621
+ are independent. Expanding the two removed quantities consequently
622
+ gives the exact formula
623
+ \begin{align}
624
+ \E_{\mathrm{graph}}\sum_{h\notin S}g\delta_hY_h
625
+ &=\sum_{i,t\in S}g^2K_{it}d_t
626
+ +\sum_{i\in S}g^2d_i\sum_{h\notin S}gq_{hi}(1-q_{hi})\notag\\
627
+ &\le\sum_{i,t\in S}g^2K_{it}d_t+gV.
628
+ \label{eq:rnd-diagonal-correction}
629
+ \end{align}
630
+ Here $\sum_hgq_{hi}=1$ bounds the diagonal correction.
631
+
632
+ For the cap contribution, the external incoming mass at $i$ is
633
+ $1-w_i=(1-y)+(y-w_i)$. Split it in these proportions. On its first
634
+ part use $b_h\le b$, and on its second part use, whenever $q_{hi}>0$,
635
+ \[
636
+ b_h\le d_h\le d_i+d(i,h)
637
+ \le d_i+(1-\widehat Pq_{hi})N_i.
638
+ \]
639
+ This yields
640
+ \begin{equation}\label{eq:rnd-backup-average}
641
+ \sum_{h\notin S}gq_{hi}b_h
642
+ \le(1-y)b+(y-w_i)\bigl[d_i+(1-\widehat Ps_i)N_i\bigr].
643
+ \end{equation}
644
+ If $w_i=1$, then $y=1$ and both sides are zero, so the convention
645
+ for $s_i$ requires no division in that case.
646
+
647
+ For completeness, averaging \eqref{eq:rnd-ideal-generator} before
648
+ using the cap bound gives, apart from the additive term $BgV$,
649
+ \begin{align*}
650
+ &[1-(1+y)a-By]V-y(1-y)b\\
651
+ &\quad+\sum_{i\in S}g\sum_{h\notin S}gq_{hi}b_h
652
+ +a\sum_{i\in S}gw_id_i+BV\sum_{i\in S}gw_i
653
+ +B\sum_{i,t\in S}g^2K_{it}d_t\\
654
+ &\quad-\sum_{i,t\in S}g^2(1-q_{ti})(d_t-ad_i)_+.
655
+ \end{align*}
656
+ The first term of \eqref{eq:rnd-backup-average}, summed over $i$,
657
+ cancels $-y(1-y)b$. The coefficient of $V$ after adding
658
+ \eqref{eq:rnd-time-derivative} simplifies using
659
+ \begin{equation}\label{eq:rnd-coefficient-identity}
660
+ (1+y)a+yB+x(y-x)B'-1=3y+B(y-x)^2.
661
+ \end{equation}
662
+ Indeed \eqref{eq:rnd-function-identities} and its derivative give
663
+ \[
664
+ (1+x)A+xB-1=3x,
665
+ \qquad A+(2+x)B+xB'=3.
666
+ \]
667
+ Expanding the left side of \eqref{eq:rnd-coefficient-identity} in
668
+ $y-x$ has these as its constant and linear coefficients, and has
669
+ quadratic coefficient $B$.
670
+
671
+ It follows that $\dot f+\E_{\mathrm{graph}}\mathcal B-BgV$ is at most
672
+ \begin{equation}\label{eq:rnd-expanded-drift}
673
+ \begin{aligned}
674
+ &-[3y+B(y-x)^2]V\\
675
+ &\quad+\sum_{i\in S}g\Bigg\{
676
+ (y-w_i)\bigl[d_i+(1-\widehat Ps_i)N_i\bigr]+aw_id_i
677
+ +BVw_i+B\sum_{t\in S}gK_{it}d_t\\
678
+ &\hspace{43mm}
679
+ -\sum_{t\in S}g(1-q_{ti})(d_t-ad_i)_+\Bigg\}.
680
+ \end{aligned}
681
+ \end{equation}
682
+
683
+ If $y=0$, the ideal generator and time derivative are zero. If
684
+ $y>0$ but $V=0$, then every $d_i$ with $i\in S$ is zero. For any
685
+ $i\in S$ with $N_i>0$, all alive sources are colocated with $i$, so
686
+ $q_{ti}=1$ for every $t\in S$ and $w_i=y$. If $N_i=0$, its radius
687
+ term already vanishes. Every term of
688
+ \eqref{eq:rnd-expanded-drift} is then zero. Thus the lemma holds
689
+ in these degenerate cases without normalization.
690
+
691
+ Assume now $V>0$, and set
692
+ \begin{equation}\label{eq:rnd-normalization}
693
+ \mu=V/y,\qquad
694
+ D_i=d_i/\mu,\qquad
695
+ r_i=w_i/y,\qquad
696
+ R_i=(1-2\zeta)N_i/\mu,\qquad C_i=1-Ps_i.
697
+ \end{equation}
698
+ Give each index $i\in S$ probability $g/y$. Expectations over these
699
+ indices, written $\E_i$ and $\E_t$, satisfy
700
+ $\E_iD_i=1$ and $r_i=\E_tq_{ti}$.
701
+ For $q=q_{ti}<1$, the taper approximation implies
702
+ \[
703
+ (1-2\zeta)(1-Pq)\le1-\widehat Pq,
704
+ \]
705
+ because the difference is at least
706
+ $2\zeta(1-Pq)-\zeta q\ge2\zeta(1-q)\ge0$.
707
+ The triangle inequality and \eqref{eq:rnd-taper-comparison} give
708
+ \begin{equation}\label{eq:rnd-normalized-comparison}
709
+ R_i(1-Pq_{ti})\le D_i+D_t\qquad(q_{ti}<1).
710
+ \end{equation}
711
+ These are precisely the radius hypotheses of
712
+ Theorem~\ref{thm:finite-inequality}.
713
+
714
+ The error in changing the taper coefficient is controlled without
715
+ any bound on individual normalized radii. Multiply the first
716
+ inequality in \eqref{eq:rnd-taper-comparison} by
717
+ $(g/y)(1-q_{ti})$, sum over $t\in S$, and use
718
+ $1-\widehat Pq_{ti}\ge1/2$ and $d(i,t)\le d_i+d_t$. This proves
719
+ \begin{equation}\label{eq:rnd-radius-error-control}
720
+ (1-r_i)N_i/\mu\le2(D_i+1).
721
+ \end{equation}
722
+ Since
723
+ \[
724
+ 0\le(1-\widehat Ps_i)-(1-2\zeta)(1-Ps_i)\le3\zeta,
725
+ \]
726
+ the replacement of
727
+ $(1-r_i)(1-\widehat Ps_i)N_i/\mu$ by
728
+ $C_i(1-r_i)R_i$ costs at most $6\zeta(D_i+1)$, whose expectation
729
+ is at most $12\zeta$.
730
+
731
+ Divide \eqref{eq:rnd-expanded-drift} by $yV=y^2\mu$ and put
732
+ $\Theta=P(y-x)^2/y$. By \eqref{eq:rnd-kernel-bound}, the normalized
733
+ kernel term is at most
734
+ \[
735
+ B\E_{i,t}K_{it}D_t
736
+ \le P\E_i\bigl[s_i(1-yr_i)(1+D_i)\bigr].
737
+ \]
738
+ After the radius replacement, the entire normalized expression is
739
+ therefore at most
740
+ \begin{align*}
741
+ -3-2\Theta+\E_i\Big[&
742
+ (1-r_i)(D_i+C_iR_i)+ar_iD_i+2Pyr_i\\
743
+ &+Ps_i(1-yr_i)(1+D_i)
744
+ -\E_t(1-q_{ti})(D_t-aD_i)_+\Big]+12\zeta.
745
+ \end{align*}
746
+ Using $a=1+m+2Py$ and $\E_iD_i=1$, this is exactly
747
+ \begin{align*}
748
+ \E_i\Big[&C_i(1-r_i)R_i
749
+ +r_i\{mD_i+(2-s_i)Py(D_i+1)\}-C_i(D_i+1)\\
750
+ &-\E_t(1-q_{ti})(D_t-(1+m+2Py)D_i)_+\Big]
751
+ -2\Theta+12\zeta.
752
+ \end{align*}
753
+ Theorem~\ref{thm:finite-inequality} bounds the expectation by
754
+ $2\Theta$. Multiplication by $yV$, with $y\le1$, proves
755
+ \[
756
+ \dot f+\E_{\mathrm{graph}}\mathcal B
757
+ \le BgV+12\zeta yV\le BgV+12\zeta V,
758
+ \]
759
+ as claimed.
760
+ \end{proof}
761
+
762
+ \subsection{Survival, accumulated error, and parameter choices}
763
+
764
+ \begin{lemma}[Decay of the alive mass]\label{lem:rnd-survival}
765
+ For sufficiently small $\ell$ depending only on $\Delta$, every
766
+ client's analysis process satisfies
767
+ \begin{equation}\label{eq:rnd-survival}
768
+ \E y_T\le(1-\ell/2)^T\le e^{-\Lambda/2}.
769
+ \end{equation}
770
+ \end{lemma}
771
+
772
+ \begin{proof}
773
+ Condition on a history, a graph, and a currently alive target.
774
+ If its group is forced, the original target identity is removed
775
+ certainly. Otherwise its $\Delta$ incoming source copies correspond
776
+ to $\Delta$ distinct possible actions: each ordinary source gives
777
+ its selection action, and each heavy source gives the unique chunk
778
+ containing this target. The marginal and pair estimates in the
779
+ proof of Lemma~\ref{lem:rnd-batch} give an erasure probability at least
780
+ \[
781
+ \Delta\ell g\bigl(1-O_\Delta(\ell)\bigr)
782
+ -O(\Delta^2\ell^2g^2)\ge\ell/2.
783
+ \]
784
+ Here the lower bound is the union bound with pair intersections
785
+ subtracted. A simultaneous reset does not restore the original
786
+ copy identity, and additional analysis discards only reduce survival.
787
+ The conditional expected surviving mass is thus at most
788
+ $(1-\ell/2)y$. Iteration, starting from $y_0=1$, and $T\ell\ge\Lambda$
789
+ prove the lemma.
790
+ \end{proof}
791
+
792
+ We finish the proof of Theorem~\ref{thm:grid-rounding}.
793
+ First run the process without rejecting count failures, and complete
794
+ every output by Lemma~\ref{lem:rnd-completion}. Average
795
+ Lemma~\ref{lem:rnd-batch} over the graph and use
796
+ Lemma~\ref{lem:rnd-average}. Since $V\le V_0$, $B\le1$, and
797
+ $R\le\Delta V_0$, summing over $T$ rounds gives
798
+ \[
799
+ \E f_T\le
800
+ \left[1+2/e+(\Lambda+1)
801
+ \{g+12\zeta+C_\Delta\Delta(\phi+\ell)\}\right]V_0
802
+ \]
803
+ for a constant $C_\Delta$, provided $\ell\le1$.
804
+ Equations~\eqref{eq:rnd-terminal-correction} and
805
+ \eqref{eq:rnd-survival} consequently imply the unconditional estimate
806
+ \begin{equation}\label{eq:rnd-total-error}
807
+ \E C_j\le
808
+ \left[1+2/e+5\Delta e^{-\Lambda/2}
809
+ +(\Lambda+1)\{g+12\zeta+C_\Delta\Delta(\phi+\ell)\}\right]V_0.
810
+ \end{equation}
811
+ All these estimates also apply when $V_0=0$: then $R=0$, the completed
812
+ connection cost is zero, and no normalization by $V_0$ is used.
813
+
814
+ Here is an explicit order of choices that avoids circular dependence.
815
+ It suffices to consider $0<\tau\le1$.
816
+ \begin{enumerate}
817
+ \item Choose a sufficiently large constant integer $\Delta$ and put
818
+ $g=1/\Delta$. For each such choice take, for example,
819
+ \[
820
+ \Lambda=\left\lceil2\log(40\Delta/\tau)\right\rceil+1.
821
+ \]
822
+ Then $5\Delta e^{-\Lambda/2}\le\tau/8$. Taking $\Delta$ sufficiently
823
+ large also makes $(\Lambda+1)g\le\tau/8$, since
824
+ $g\log(1/g)\longrightarrow0$. Any additional upper bound on $g$
825
+ required by the preparation stage may be imposed at the same time.
826
+ \item With $\Delta,\Lambda$ fixed, choose a small positive rational
827
+ $\zeta$ so that $12(\Lambda+1)\zeta\le\tau/8$.
828
+ Next choose a small positive rational $\phi$, and then a small positive
829
+ rational $\ell$, so that
830
+ \[
831
+ C_\Delta\Delta(\Lambda+1)(\phi+\ell)\le\tau/8.
832
+ \]
833
+ Require in addition every upper bound on $\ell$ used in the count,
834
+ batch, and survival lemmas, and $p_*(1+\phi)\le1$.
835
+ The batch constants are uniform in the remaining threshold $b_*$,
836
+ so these requirements can be imposed before choosing that threshold.
837
+ This fixes the constant number of rounds $T=\lceil\Lambda/\ell\rceil$.
838
+ \item Put $\alpha=1+2/e$ and choose a fixed
839
+ $0<\eta\le\tau/(4(\alpha+\tau))$.
840
+ Finally choose rational $b_*>0$ as in Lemma~\ref{lem:rnd-count} so
841
+ that the final mass is at most $M+C$ with probability at least
842
+ $1-\eta$.
843
+ \end{enumerate}
844
+ The unconditional cost in \eqref{eq:rnd-total-error} is then at most
845
+ $(\alpha+\tau/2)V_0$ for every client. Repeat the entire process on
846
+ failure of the final mass test. The accepted output is the
847
+ unconditional output conditioned on that test, whose success
848
+ probability is at least $1-\eta$. Since connection costs are
849
+ nonnegative,
850
+ \[
851
+ \E[C_j\mid\text{mass test succeeds}]
852
+ \le\frac{\alpha+\tau/2}{1-\eta}V_0
853
+ \le(\alpha+\tau)V_0.
854
+ \]
855
+ Completion uses at most the final active mass, so an accepted output
856
+ has at most $M+C$ facilities. This proves the count and cost assertions
857
+ of Theorem~\ref{thm:grid-rounding}.
858
+
859
+ For fixed accuracy all parameters are instance-independent constants.
860
+ The number of current facilities never exceeds the number in the
861
+ split input, and every group has at most $\Delta$ active copies.
862
+ The graph, its marginals, a fixed-sum rounding, the action sets,
863
+ their intersections, and the greedy completion can therefore be
864
+ computed in polynomial time. The radius equations and all physical
865
+ probabilities are rational; the approximations in
866
+ \eqref{eq:rnd-taper-approximation} are fixed constants. Only the
867
+ analysis uses the transcendental functions or alive-set discards.
868
+ The expected number of repetitions is at most $1/(1-\eta)$, giving
869
+ expected polynomial running time. Section~\ref{sec:derandomization}
870
+ replaces the local random choices by polynomial-size lists and obtains
871
+ a deterministic output with the corresponding total-cost bound.
preprints/The-Approximation-Threshold-for-Metric-k-Median-September-24-2026/main.pdf ADDED
@@ -0,0 +1,3 @@
 
 
 
 
1
+ version https://git-lfs.github.com/spec/v1
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+ oid sha256:c8176d1671beb83d3a459ff65e5c632d94364ec7e542930bf19fad0b75524d50
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+ size 562378
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [The Artinian Lex-Plus-Powers Betti Theorem](paper.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** September 23, 2026
6
+
7
+ ## Citation
8
+
9
+ ```bibtex
10
+ @misc{OAI:The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026,
11
+ author = {{OpenAI}},
12
+ title = {{The Artinian Lex-Plus-Powers Betti Theorem}},
13
+ howpublished = {OpenAI Math Release preprint
14
+ \href{https://github.com/openai/math/blob/main/preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/paper.pdf}{OAI:The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026}},
15
+ year = {2026}
16
+ }
17
+ ```
18
+
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/bibliography.tex ADDED
@@ -0,0 +1,130 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \begin{thebibliography}{99}
2
+ \bibitem{Abedelfatah15}
3
+ A.~Abedelfatah,
4
+ \emph{On the Eisenbud--Green--Harris conjecture},
5
+ Proc. Amer. Math. Soc. \textbf{143} (2015), no.~1, 105--115.
6
+ \href{https://doi.org/10.1090/S0002-9939-2014-12216-7}{doi:10.1090/S0002-9939-2014-12216-7}.
7
+ Numbered statements refer to
8
+ \href{https://arxiv.org/abs/1212.2653v1}{arXiv:1212.2653v1}.
9
+
10
+ \bibitem{Bigatti}
11
+ A.~M.~Bigatti,
12
+ \emph{Upper bounds for the Betti numbers of a given Hilbert function},
13
+ Comm.\ Algebra \textbf{21} (1993), no.~7, 2317--2334.
14
+ \href{https://doi.org/10.1080/00927879308824679}{doi:10.1080/00927879308824679}.
15
+
16
+ \bibitem{BCR}
17
+ A.~M.~Bigatti, A.~Conca, and L.~Robbiano,
18
+ \emph{Generic initial ideals and distractions},
19
+ Comm.\ Algebra \textbf{33} (2005), no.~6, 1709--1732.
20
+ \href{https://doi.org/10.1081/AGB-200058217}{doi:10.1081/AGB-200058217}.
21
+ Author version:
22
+ \href{https://arxiv.org/abs/math/0308004}{arXiv:math/0308004}.
23
+
24
+ \bibitem{CDeS20}
25
+ G.~Caviglia and A.~De Stefani,
26
+ \emph{The Eisenbud--Green--Harris conjecture for fast-growing degree sequences},
27
+ Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) \textbf{25} (2024), no.~3,
28
+ 1753--1762.
29
+ \href{https://doi.org/10.2422/2036-2145.202203_025}{doi:10.2422/2036-2145.202203\_025}.
30
+ Numbered statements refer to
31
+ \href{https://arxiv.org/abs/2007.15467v2}{arXiv:2007.15467v2}.
32
+
33
+ \bibitem{CK14}
34
+ G.~Caviglia and M.~Kummini,
35
+ \emph{Poset embeddings of Hilbert functions and Betti numbers},
36
+ J. Algebra \textbf{410} (2014), 244--257.
37
+ \href{https://doi.org/10.1016/j.jalgebra.2014.04.007}{doi:10.1016/j.jalgebra.2014.04.007}.
38
+ Numbered statements refer to
39
+ \href{https://arxiv.org/abs/1210.5562v2}{arXiv:1210.5562v2}.
40
+
41
+ \bibitem{CM08}
42
+ G.~Caviglia and D.~Maclagan,
43
+ \emph{Some cases of the Eisenbud--Green--Harris conjecture},
44
+ Math. Res. Lett. \textbf{15} (2008), no.~3, 427--433.
45
+ \href{https://www.math.purdue.edu/~gcavigli/Articles-PDF/%5B4%5D.pdf}{Author manuscript}.
46
+
47
+ \bibitem{CS}
48
+ G.~Caviglia and A.~Sammartano,
49
+ \emph{On the Lex-plus-powers Conjecture},
50
+ Adv.\ Math.\ \textbf{340} (2018), 284--299.
51
+ \href{https://doi.org/10.1016/j.aim.2018.10.005}{doi:10.1016/j.aim.2018.10.005}.
52
+ Numbered statements refer to
53
+ \href{https://arxiv.org/abs/1802.03035v2}{arXiv:1802.03035v2}.
54
+
55
+ \bibitem{CL}
56
+ G.~F.~Clements and B.~Lindstr\"om,
57
+ \emph{A generalization of a combinatorial theorem of Macaulay},
58
+ J. Combin. Theory \textbf{7} (1969), no.~3, 230--238.
59
+ \href{https://doi.org/10.1016/S0021-9800(69)80016-5}{doi:10.1016/S0021-9800(69)80016-5}.
60
+
61
+ \bibitem{EGH}
62
+ D.~Eisenbud, M.~Green, and J.~Harris,
63
+ \emph{Higher Castelnuovo theory},
64
+ Ast\'erisque \textbf{218} (1993), 187--202.
65
+ \url{https://www.numdam.org/item/AST_1993__218__187_0/}.
66
+
67
+ \bibitem{FR}
68
+ C.~A.~Francisco and B.~P.~Richert,
69
+ \emph{Lex-plus-powers ideals},
70
+ in I.~Peeva (ed.), \emph{Syzygies and Hilbert Functions},
71
+ Lecture Notes in Pure and Applied Mathematics \textbf{254},
72
+ Chapman \& Hall/CRC, Boca Raton, FL, 2007, 113--144.
73
+ Author version:
74
+ \url{https://math.okstate.edu/people/chris/lpp-updated-final.pdf}.
75
+
76
+ \bibitem{Hulett}
77
+ H.~A.~Hulett,
78
+ \emph{Maximum Betti numbers of homogeneous ideals with a given Hilbert function},
79
+ Comm.\ Algebra \textbf{21} (1993), no.~7, 2335--2350.
80
+ \href{https://doi.org/10.1080/00927879308824680}{doi:10.1080/00927879308824680}.
81
+
82
+ \bibitem{Kuzmanovski}
83
+ N.~Kuzmanovski,
84
+ \emph{A Structural Property of Generic Initial Ideals},
85
+ preprint, 18 August 2026.
86
+ \href{https://arxiv.org/abs/2608.17281v1}{arXiv:2608.17281v1}.
87
+
88
+ \bibitem{MM}
89
+ J.~Mermin and S.~Murai,
90
+ \emph{The Lex-Plus-Powers Conjecture holds for pure powers},
91
+ Adv.\ Math.\ \textbf{226} (2011), no.~4, 3511--3539.
92
+ \href{https://doi.org/10.1016/j.aim.2010.08.022}{doi:10.1016/j.aim.2010.08.022}.
93
+ Author version: \url{https://s-murai.w.waseda.jp/papers/LPP.pdf}.
94
+
95
+ \bibitem{MPS}
96
+ J.~Mermin, I.~Peeva, and M.~Stillman,
97
+ \emph{Ideals containing the squares of the variables},
98
+ Adv.\ Math.\ \textbf{217} (2008), no.~5, 2206--2230.
99
+ \href{https://doi.org/10.1016/j.aim.2007.11.014}{doi:10.1016/j.aim.2007.11.014}.
100
+ Author version:
101
+ \url{https://pi.math.cornell.edu/~mermin/papers/ideals_containing_the_squares_of_the_variables.pdf}.
102
+
103
+ \bibitem{Murai}
104
+ S.~Murai,
105
+ \emph{Borel-plus-powers monomial ideals},
106
+ J. Pure Appl. Algebra \textbf{212} (2008), no.~6, 1321--1336.
107
+ \href{https://doi.org/10.1016/j.jpaa.2007.09.010}{doi:10.1016/j.jpaa.2007.09.010}.
108
+ Author version: \url{https://s-murai.w.waseda.jp/papers/BPP.pdf}.
109
+
110
+ \bibitem{ArtinianEGH}
111
+ OpenAI,
112
+ \emph{Commuting Division-Coefficient Forms and the Artinian
113
+ Eisenbud--Green--Harris Conjecture},
114
+ OpenAI Math Release preprint
115
+ \href{https://github.com/openai/math/blob/main/preprints/Commuting-Division-Coefficient-Forms-and-the-Artinian-Eisenbud-Green-Harris-Conjecture-September-23-2026/paper.pdf}{OAI:Commuting-Division-Coefficient-Forms-and-the-Artinian-Eisenbud-Green-Harris-Conjecture-September-23-2026},
116
+ 2026.
117
+
118
+ \enlargethispage{2\baselineskip}
119
+ \bibitem{Pardue}
120
+ K.~Pardue,
121
+ \emph{Deformation classes of graded modules and maximal Betti numbers},
122
+ Illinois J. Math.\ \textbf{40} (1996), no.~4, 564--585.
123
+ \href{https://doi.org/10.1215/ijm/1255985937}{doi:10.1215/ijm/1255985937}.
124
+
125
+ \bibitem{Richert}
126
+ B.~P.~Richert,
127
+ \emph{A study of the lex plus powers conjecture},
128
+ J. Pure Appl. Algebra \textbf{186} (2004), no.~2, 169--183.
129
+ \href{https://doi.org/10.1016/S0022-4049(03)00130-0}{doi:10.1016/S0022-4049(03)00130-0}.
130
+ \end{thebibliography}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/figures/endpoint-slices.tex ADDED
@@ -0,0 +1,22 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \begin{figure}[htbp]
2
+ \centering
3
+ \begin{tikzpicture}[>=Stealth,font=\small]
4
+ \node (u) at (-3.3,0) {$uz^s\in H$};
5
+ \node (xu) at (3.3,0) {$x_iuz^s\in zH$};
6
+ \node (transfer) at (3.3,-1.5) {$x_iuz^{s-1}\in H$};
7
+ \draw[->] (u) -- node[above] {$\times x_i$} (xu);
8
+ \draw[->] (transfer) -- node[right] {$\times z$} (xu);
9
+ \draw[->,dashed] (u) --
10
+ node[pos=.47,below,sloped] {transfer $z$ to $x_i$} (transfer);
11
+ \node[align=center] at (-3.2,-1.55)
12
+ {$x_i[uz^s]=0$ in $H/zH$\\[3pt]
13
+ $1\le s<a$};
14
+ \end{tikzpicture}
15
+ \caption{A middle slice is annihilated by every earlier variable.
16
+ The dashed arrow is supplied by box stability, or by an earlier
17
+ prescribed power if the monomial leaves the earlier-variable box.
18
+ Consequently all Koszul differentials on a middle slice vanish.
19
+ At $s=0$ there is no factor of $z$ to transfer; at $s=a$ the
20
+ last exponent is outside the box. These are the two endpoints.}
21
+ \label{fig:endpoint-slices}
22
+ \end{figure}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/main.tex ADDED
@@ -0,0 +1,64 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \pdfminorversion=7
2
+ \documentclass[11pt]{article}
3
+ \usepackage[T1]{fontenc}
4
+ \usepackage{lmodern}
5
+ \usepackage[margin=1in]{geometry}
6
+ \usepackage{amsmath,amssymb,amsthm,mathtools}
7
+ \usepackage{microtype}
8
+ \usepackage{enumitem}
9
+ \usepackage{xcolor}
10
+ \usepackage{tikz}
11
+ \usetikzlibrary{arrows.meta,positioning}
12
+ \definecolor{linkblue}{RGB}{26,65,110}
13
+ \PassOptionsToPackage{hyphens}{url}
14
+ \usepackage[colorlinks=true,linkcolor=linkblue,citecolor=linkblue,urlcolor=linkblue]{hyperref}
15
+ \hypersetup{pdftitle={The Artinian Lex-Plus-Powers Betti Theorem},pdfauthor={OpenAI}}
16
+ \pdfinfoomitdate=1
17
+ \pdftrailerid{}
18
+ \pdfsuppressptexinfo=15
19
+ \setlength{\emergencystretch}{2em}
20
+ \setlist{itemsep=3pt,topsep=5pt}
21
+ \newtheorem{theorem}{Theorem}[section]
22
+ \newtheorem{proposition}[theorem]{Proposition}
23
+ \newtheorem{lemma}[theorem]{Lemma}
24
+ \newtheorem{corollary}[theorem]{Corollary}
25
+ \theoremstyle{definition}
26
+ \newtheorem{definition}[theorem]{Definition}
27
+ \theoremstyle{remark}
28
+ \newtheorem{remark}[theorem]{Remark}
29
+ \numberwithin{equation}{section}
30
+ \newcommand{\C}{\mathbb C}
31
+ \newcommand{\N}{\mathbb Z_{\ge0}}
32
+ \newcommand{\Z}{\mathbb Z}
33
+ \newcommand{\Q}{\mathbb Q}
34
+ \DeclareMathOperator{\Tor}{Tor}
35
+ \DeclareMathOperator{\Hilb}{Hilb}
36
+ \DeclareMathOperator{\Lex}{Lex}
37
+ \DeclareMathOperator{\rank}{rank}
38
+ \DeclareMathOperator{\Sym}{Sym}
39
+ \DeclareMathOperator{\inm}{in}
40
+ \title{The Artinian Lex-Plus-Powers Betti Theorem}
41
+ \author{OpenAI}
42
+ \date{September 23, 2026}
43
+ \begin{document}
44
+ \maketitle
45
+ \begin{abstract}
46
+ We prove the Eisenbud--Green--Harris and lex-plus-powers conjectures over every
47
+ characteristic-zero field for homogeneous regular sequences of any positive
48
+ length, with degrees at least two. For every homogeneous ideal containing such
49
+ a sequence, the corresponding lex-plus-powers ideal has the same Hilbert
50
+ function and at least as large a graded Betti number in every homological and
51
+ internal degree.
52
+ \end{abstract}
53
+ \tableofcontents
54
+ \input{sections/01-introduction}
55
+ \input{sections/01-forms}
56
+ \input{sections/02-filtered}
57
+ \input{sections/03-monomial}
58
+ \input{sections/04-stabilization}
59
+ \input{sections/05-boxes}
60
+ \input{sections/06-tor}
61
+ \input{sections/07-assembly}
62
+ \input{sections/08-characteristic-zero}
63
+ \input{bibliography}
64
+ \end{document}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/01-forms.tex ADDED
@@ -0,0 +1,48 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Commuting forms with division coefficients}\label{sec:forms}
2
+
3
+ We state the construction theorem from the companion article
4
+ \cite{ArtinianEGH} in the precise form used below. A central
5
+ division algebra over \(k\) is a finite-dimensional
6
+ \(k\)-algebra with center \(k\) in which every nonzero element is invertible.
7
+ In \(\Delta[x]\), the variables \(x_i\) are central and have degree one,
8
+ and elements of \(\Delta\) have degree zero.
9
+
10
+ \begin{theorem}[Commuting-form construction, {\cite[Theorem~1.1]{ArtinianEGH}}]
11
+ \label{thm:forms}
12
+ Let \(f_1,\ldots,f_n\) be a homogeneous regular sequence in
13
+ \(\C[x_1,\ldots,x_n]\), of degrees \(2\le a_1\le\cdots\le a_n\).
14
+ There are a field extension \(k/\C\), a central division \(k\)-algebra
15
+ \(\Delta\), and a commutative graded \(k\)-subalgebra
16
+ \[
17
+ k[x_1,\ldots,x_n]\subseteq A\subseteq N=\Delta[x_1,\ldots,x_n]
18
+ \]
19
+ generated by finitely many elements of degree one, containing
20
+ \(t_1,\ldots,t_n\in A_1\), such that
21
+ \begin{equation}\label{eq:triangular-forms}
22
+ t_h^{a_h}=c_h f_h+\sum_{\ell<h}B_{h\ell}f_\ell
23
+ +\sum_{\ell>h}C_{h\ell}t_\ell
24
+ \qquad(1\le h\le n).
25
+ \end{equation}
26
+ Here \(c_h\in k^\times\), \(B_{h\ell},C_{h\ell}\in A\), and every summand
27
+ has degree \(a_h\). Moreover,
28
+ \[
29
+ \{t^\alpha=t_1^{\alpha_1}\cdots t_n^{\alpha_n}:
30
+ \alpha\in\N^n\}
31
+ \]
32
+ is a graded left-\(\Delta\) basis of the \emph{full} algebra \(N\).
33
+ \end{theorem}
34
+
35
+ The basis assertion in Theorem~\ref{thm:forms} is stronger than a basis of the finite
36
+ complete-intersection quotient: every monomial \(t^\alpha\), without
37
+ an upper bound on its exponents, occurs in the decomposition of \(N\).
38
+ This is what will make \(N\) a free module over a polynomial ring and
39
+ allow us to transfer an entire resolution. The Hilbert-function
40
+ consequence of the foundation theorem alone would not suffice.
41
+
42
+ \begin{remark}\label{rem:coefficients}
43
+ Commutativity of the forms does not mean that their individual
44
+ \(\Delta\)-coefficients commute. The proof below always places those
45
+ coefficients on the left and multiplies by the \(t_i\) on the right.
46
+ The construction itself has no hypothesis on the additional generators
47
+ of \(I\).
48
+ \end{remark}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/01-introduction.tex ADDED
@@ -0,0 +1,227 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Introduction}\label{sec:introduction}
2
+
3
+ A Hilbert function records the dimensions of a graded quotient; its graded
4
+ Betti numbers also record the relations among its generators and all higher
5
+ syzygies. The lex-plus-powers conjecture predicts one extremal ideal for
6
+ both kinds of data when the original ideal contains a regular sequence.
7
+ We prove its full Artinian form over \(\C\), and deduce the full
8
+ characteristic-zero statement for regular sequences of arbitrary positive
9
+ length by the established Artinian reduction and coefficient-field descent.
10
+
11
+ Let
12
+ \[
13
+ S=\C[x_1,\ldots,x_n],\qquad
14
+ 2\le a_1\le\cdots\le a_n,\qquad
15
+ P=(x_1^{a_1},\ldots,x_n^{a_n}),
16
+ \]
17
+ where each variable has degree one. Lexicographic order always has
18
+ \(x_1>\cdots>x_n\), and a lex segment starts with the \emph{greatest}
19
+ monomials. Suppose that a homogeneous ideal \(I\subseteq S\) contains a
20
+ homogeneous regular sequence \(f_1,\ldots,f_n\) with \(\deg f_i=a_i\).
21
+ Here regularity means that multiplication by \(f_i\) is injective on
22
+ \(S/(f_1,\ldots,f_{i-1})\) for each \(i\). Its full length makes
23
+ \(S/I\) Artinian: the complete-intersection Hilbert series is
24
+ \(\prod_i(1+z+\cdots+z^{a_i-1})\).
25
+ For each \(d\ge0\), prescribe
26
+ \begin{equation}
27
+ J_d=L_d+P_d,\qquad \dim_\C J_d=\dim_\C I_d,
28
+ \label{eq:prescription}
29
+ \end{equation}
30
+ where \(L_d\) is the largest lex-segment subspace with this property.
31
+ Part of the assertion below is that these dimensions can be attained
32
+ and that the prescribed spaces form an ideal.
33
+
34
+ For a standard graded polynomial ring \(A\) over a field \(F\), write
35
+ \[
36
+ \beta^A_{p,j}(B)=\dim_F\Tor^A_p(B,F)_j,
37
+ \qquad F=A/A_{>0}.
38
+ \]
39
+ The index \(p\) is the homological degree and \(j\) is the internal degree.
40
+
41
+ \begin{theorem}\label{thm:main}
42
+ For every \(n\ge1\), every ordered degree sequence
43
+ \(2\le a_1\le\cdots\le a_n\), and every homogeneous ideal
44
+ \(I\subseteq\C[x_1,\ldots,x_n]\) containing a regular sequence of these
45
+ degrees, the spaces in \eqref{eq:prescription} exist and
46
+ \(J=\bigoplus_{d\ge0}J_d\) is a homogeneous ideal. For this single ideal,
47
+ \[
48
+ \beta^S_{p,j}(S/I)\le\beta^S_{p,j}(S/J)
49
+ \qquad\text{for every \(p\ge0\) and \(j\in\Z\)}.
50
+ \]
51
+ There is no restriction on the degrees or number of the additional
52
+ generators of \(I\).
53
+ \end{theorem}
54
+
55
+ Thus Theorem~\ref{thm:main} resolves the Artinian lex-plus-powers
56
+ conjecture positively over \(\C\).
57
+ Its Hilbert-function assertion is the Artinian Eisenbud--Green--Harris
58
+ statement; the Betti inequalities are stronger.
59
+
60
+ The Artinian restriction can be removed from these two conclusions.
61
+ Caviglia and Maclagan proved the Artinian reduction for the
62
+ Eisenbud--Green--Harris conjecture \cite[Proposition~10]{CM08};
63
+ Caviglia and Kummini proved the corresponding reduction for
64
+ lex-plus-powers Betti numbers \cite[Section~4, Theorem~4.1]{CK14}.
65
+ Together with a finite coefficient-field descent, these reductions give
66
+ the following form over every characteristic-zero field.
67
+
68
+ \begin{corollary}[Eisenbud--Green--Harris and lex-plus-powers in characteristic zero]
69
+ \label{cor:characteristic-zero}
70
+ Let \(F\) be a field of characteristic zero, let
71
+ \[
72
+ S_F=F[x_1,\ldots,x_n],\qquad
73
+ 1\le c\le n,\qquad 2\le a_1\le\cdots\le a_c,
74
+ \qquad P_F=(x_1^{a_1},\ldots,x_c^{a_c}),
75
+ \]
76
+ with the standard grading and lexicographic order \(x_1>\cdots>x_n\).
77
+ Suppose that a homogeneous ideal \(I\subseteq S_F\) contains a homogeneous
78
+ regular sequence \(f_1,\ldots,f_c\) with \(\deg f_i=a_i\).
79
+ For \(d\ge0\), put
80
+ \[
81
+ q_d=\dim_F I_d-\dim_F(P_F)_d.
82
+ \]
83
+ This integer lies between zero and the number of degree-\(d\) monomials
84
+ outside \(P_F\). Let \(J_d\) be the sum of \((P_F)_d\) and the span of the
85
+ \(q_d\) lexicographically greatest such monomials. Then
86
+ \(J=\bigoplus_{d\ge0}J_d\) is a homogeneous ideal, and for this single ideal
87
+ \[
88
+ \dim_F(S_F/I)_d=\dim_F(S_F/J)_d\quad(d\ge0),\qquad
89
+ \beta^{S_F}_{p,j}(S_F/I)\le\beta^{S_F}_{p,j}(S_F/J)
90
+ \quad(p\ge0,\ j\in\Z).
91
+ \]
92
+ There is no restriction on the degrees or number of the additional
93
+ generators of \(I\).
94
+ \end{corollary}
95
+
96
+ Corollary~\ref{cor:characteristic-zero} includes non-Artinian quotients
97
+ and fields that are not algebraically closed. The case with no prescribed
98
+ regular sequence is the classical lex-ideal theorem cited below.
99
+ The division-coefficient construction itself remains the full-length
100
+ construction over \(\C\); Section~\ref{sec:characteristic-zero} proves
101
+ the corollary from Theorem~\ref{thm:main}.
102
+
103
+ \subsection{Context and previous results}
104
+
105
+ The Eisenbud--Green--Harris (EGH) Hilbert-function conjecture arose in
106
+ their work on higher Castelnuovo theory \cite[Section~4]{EGH}.
107
+ The lex-plus-powers conjecture, generally attributed to Charalambous
108
+ and Evans, strengthens that prediction to graded Betti numbers.
109
+ Francisco and Richert discuss its origins and identify its first
110
+ printed appearance in the work of Evans and Richert
111
+ \cite[Section~5]{FR}; see also the public formulations in
112
+ \cite[Section~1]{Richert} and
113
+ \cite[Conjectures~1.1 and 1.2]{CS}.
114
+ Without a prescribed regular sequence, the extremality of lex ideals
115
+ at fixed Hilbert function is the theorem of Bigatti, Hulett, and
116
+ Pardue \cite{Bigatti,Hulett,Pardue}.
117
+ The additional powers encode the degrees of the regular sequence and
118
+ give the sharper comparison studied here.
119
+ For ideals already containing these powers, Clements--Lindstr\"om
120
+ compression supplies the Hilbert-function comparison \cite{CL}.
121
+
122
+ The prescribed-powers Betti comparison developed through several stages.
123
+ Mermin, Peeva, and Stillman proved the comparison for ideals containing
124
+ the squares of the variables in characteristic zero
125
+ \cite[Theorem~1.1]{MPS}; Murai established it for strongly stable ideals
126
+ plus the prescribed powers over any field \cite[Theorem~1.1]{Murai}.
127
+ Mermin and Murai then proved the lex-plus-powers comparison for ideals
128
+ containing a monomial regular sequence, again over every field
129
+ \cite[Theorems~3.1 and 8.1]{MM}. They also isolated the reduction to a
130
+ Hilbert-matching monomial ideal with no smaller graded Betti numbers
131
+ \cite[Conjecture~10.2]{MM}. It is this reduction that we obtain from
132
+ division coefficients. Our proof of the subsequent monomial comparison
133
+ is included for completeness; its conclusion is not new.
134
+
135
+ For nonmonomial regular sequences, the Hilbert-function and Betti problems
136
+ have had different ranges of known cases. Abedelfatah proved EGH for full
137
+ regular sequences whose forms split into linear factors
138
+ \cite[Corollary~4.3]{Abedelfatah15}. Caviglia and Maclagan established
139
+ EGH for fast-growing degrees \cite{CM08}, and Caviglia and De Stefani
140
+ weakened the required growth to
141
+ \(a_i\ge\sum_{j<i}(a_j-1)\) for \(i\ge3\)
142
+ \cite[Theorem~A]{CDeS20}. These Hilbert-function results hold over any
143
+ field. The characteristic-zero Betti theorem of Caviglia and Sammartano
144
+ requires
145
+ \(a_i\ge1+\sum_{j<i}(a_j-1)\) for \(i\ge3\)
146
+ \cite[Theorem~3.8]{CS}. No such growth condition is imposed here.
147
+
148
+ More recently, Kuzmanovski \cite[Theorem~1.9]{Kuzmanovski} obtained
149
+ asymptotic Betti estimates in characteristic zero in a bounded degree range,
150
+ for fixed regular-sequence degree offsets and generator counts and
151
+ sufficiently large initial degree. That comparison uses the
152
+ reverse-lexicographic generic initial ideal of a lex-plus-powers ideal,
153
+ rather than the lex-plus-powers ideal itself as in Theorem~\ref{thm:main}.
154
+
155
+ Our treatment of the monomial comparison retains the
156
+ resolution-level mechanism of distractions
157
+ \cite[Theorem~2.19 and Corollary~2.20]{BCR} and the endpoint
158
+ decomposition for stable-plus-powers ideals
159
+ \cite[Lemma~3.7]{CS}, while organizing the last comparison through ranks
160
+ in the Koszul complex.
161
+
162
+ \subsection{The reduction that carries the Betti numbers}
163
+
164
+ The essential step is to find a monomial ideal \(M\supseteq P\) such that
165
+ \begin{equation}\label{eq:overview-bound}
166
+ \Hilb(S/I)=\Hilb(S/M),\qquad
167
+ \beta^S_{p,j}(S/I)\le\beta^S_{p,j}(S/M)
168
+ \quad\text{for all \(p,j\)}.
169
+ \end{equation}
170
+ Matching Hilbert functions alone cannot give the second conclusion.
171
+
172
+ Theorem~1.1 of the companion article \cite{ArtinianEGH} supplies a field
173
+ \(k/\C\), a finite-dimensional central division \(k\)-algebra \(\Delta\), and commuting linear
174
+ forms \(t_1,\ldots,t_n\) in \(N=\Delta[x_1,\ldots,x_n]\). They satisfy
175
+ triangular power identities adapted to the \(f_i\), and their ordered
176
+ monomials form a left-\(\Delta\) basis of \(N\).
177
+ Section~\ref{sec:forms} states exactly the input needed here, including
178
+ the basis assertion for the full algebra rather than only its
179
+ complete-intersection quotient.
180
+
181
+ Let \(T=k[y_1,\ldots,y_n]\) act on \(N\) on the right by \(y_i\mapsto t_i\).
182
+ Then \(N\) is simultaneously left-\(S\) free and right-\(T\) free, the
183
+ latter of rank \(m=\dim_k\Delta\), with generators in degree zero.
184
+ A minimal \(S\)-resolution of \(S/I\) therefore gives a
185
+ \emph{minimal} \(T\)-resolution of \(N/IN\), multiplying every Betti number
186
+ by the same factor \(m\). With a monomial order adapted to the triangular
187
+ identities, the leading coefficient spaces of \(IN\) in the
188
+ \(t^\alpha\)-expansion are left ideals of \(\Delta\), hence either zero
189
+ or all of \(\Delta\). Their nonzero positions define \(M\); the
190
+ triangular identities ensure that \(M\) contains \(P\). A filtered
191
+ Koszul comparison then gives \eqref{eq:overview-bound} after cancelling
192
+ \(m\).
193
+ This resolution transfer is the additional ingredient beyond the
194
+ Hilbert-function reduction in \cite{ArtinianEGH}.
195
+
196
+ Starting from \(M\), we work with the monomials in the exponent box
197
+ \(0\le u_i<a_i\). A transfer replaces a factor \(x_\ell\) by \(x_h\),
198
+ where \(h<\ell\), provided the result remains in the box.
199
+ Root-of-unity distractions followed by initial ideals produce an ideal
200
+ \(H\supseteq P\) closed under these transfers, with unchanged Hilbert
201
+ function and no smaller quotient Betti numbers. In each degree, replace
202
+ the box monomials belonging to \(H\) by the same number of greatest
203
+ lexicographic monomials in the box, and retain \(P\). Comparing their bounded
204
+ shadows---the multiples by one variable that remain in the box---shows
205
+ that the resulting space \(G\) is an ideal.
206
+
207
+ For the Betti comparison, put \(z=x_n\). The modules \(H/zH\) and
208
+ \(G/zG\) over the earlier variables have equal Hilbert functions and
209
+ retain the Betti numbers of the ideals \(H\) and \(G\). They split
210
+ into components according to the exponent of \(z\), from \(0\) to
211
+ \(a_n\). Stability makes every earlier variable annihilate the
212
+ components at exponents \(1,\ldots,a_n-1\). Only the two extreme
213
+ components can therefore contribute nonzero ranks to the Koszul
214
+ differentials. The comparisons on the box slices \(u_n=0\) and
215
+ \(u_n=a_n-1\), induction in the number of variables, and monotonicity
216
+ of differential ranks under submodules and quotients compare these
217
+ endpoint contributions. Since the Koszul terms have equal dimensions,
218
+ the resulting reverse inequality for adjacent rank sums gives the
219
+ required Betti bound.
220
+
221
+ Sections~\ref{sec:filtered} and \ref{sec:monomial} establish the filtered
222
+ comparison and the transfer to \(M\).
223
+ Sections~\ref{sec:stabilization}--\ref{sec:tor} give the complete monomial
224
+ comparison. Section~\ref{sec:assembly} identifies its output with
225
+ \eqref{eq:prescription} and proves Theorem~\ref{thm:main}.
226
+ Section~\ref{sec:characteristic-zero} then removes the Artinian and
227
+ complex-coefficient restrictions from the Hilbert and Betti conclusions.
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/02-filtered.tex ADDED
@@ -0,0 +1,231 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Graded resolutions and leading coefficient spaces}
2
+ \label{sec:filtered}
3
+
4
+ We first prove a comparison for quotients of a free module whose monomial
5
+ positions have vector-space coefficients. The application in the next
6
+ section will use a division algebra as that coefficient space. The
7
+ comparison must retain each internal degree separately, so we work with
8
+ the graded Koszul complex throughout.
9
+
10
+ Let $F$ be a field and let $A=F[y_1,\ldots,y_r]$, with each variable of
11
+ degree one. For a finitely generated graded $A$-module $B$, put
12
+ \[
13
+ \beta^A_{p,j}(B)=\dim_F\Tor^A_p(B,F)_j,
14
+ \qquad F=A/(y_1,\ldots,y_r).
15
+ \]
16
+ We use the shift convention $B(-s)_d=B_{d-s}$. All modules considered
17
+ below are bounded below and have finite-dimensional graded components.
18
+
19
+ \begin{lemma}[Minimal graded resolutions]
20
+ \label{filt:minimal}
21
+ Every finitely generated graded $A$-module $B$ has a graded free resolution
22
+ whose differentials have entries in $A_{>0}$. In such a resolution, the
23
+ number of free generators of degree $j$ in homological position $p$ is
24
+ $\beta^A_{p,j}(B)$. If $H\subsetneq A$ is a homogeneous ideal, then
25
+ \begin{equation}
26
+ \beta^A_{p+1,j}(A/H)=\beta^A_{p,j}(H)
27
+ \qquad(p\geq 0,\ j\in\Z).
28
+ \label{filt:ideal-quotient}
29
+ \end{equation}
30
+ If $H$ is monomial, a minimal resolution of $A/H$ can be chosen
31
+ homogeneous for the exponent multigrading, with all generator
32
+ multidegrees in $\Z_{\geq0}^r$.
33
+ \end{lemma}
34
+
35
+ \begin{proof}
36
+ Lift a homogeneous $F$-basis of $B/A_{>0}B$ to $B$ and map the free module
37
+ on these lifts to $B$. This map is surjective: in each degree, an element
38
+ not yet expressed in the lifts differs from such an expression by a sum
39
+ of positive-degree multiples of elements of smaller degree, to which
40
+ induction applies. Its kernel is finitely generated because $A$ is
41
+ Noetherian. Repeating the construction for successive kernels gives a
42
+ free resolution. At each stage, reduction modulo $A_{>0}$ identifies the
43
+ chosen free generators with a basis of the corresponding module modulo
44
+ $A_{>0}$, so the next kernel lies in $A_{>0}$ times that free module.
45
+ Thus every differential between free modules has positive-degree
46
+ entries. Tensoring with $F$ makes these differentials zero and proves
47
+ the assertion about $\Tor$.
48
+
49
+ A minimal resolution of a proper homogeneous ideal $H$, followed by
50
+ the inclusion $H\hookrightarrow A$ and the quotient $A\twoheadrightarrow
51
+ A/H$, is a minimal resolution of $A/H$: the additional entries also
52
+ have positive degree since $H\subseteq A_{>0}$. This proves
53
+ \eqref{filt:ideal-quotient}, including $H=0$.
54
+
55
+ For a monomial quotient, carry out the same construction with
56
+ multihomogeneous lifts. The initial free module is $A$ in multidegree
57
+ zero. A free module whose generator multidegrees are nonnegative has
58
+ no component in a multidegree outside $\Z_{\geq0}^r$; neither does its
59
+ kernel or a quotient of that kernel. Induction therefore gives the
60
+ last assertion.
61
+ \end{proof}
62
+
63
+ \begin{lemma}[Koszul calculation]
64
+ \label{filt:koszul}
65
+ Let $K_\bullet(B)$ be the Koszul complex on $y_1,\ldots,y_r$ with
66
+ coefficients in $B$. Its term of internal degree $j$ in position $p$ is
67
+ \[
68
+ K_p(B)_j=\bigoplus_{\substack{\sigma\subseteq\{1,\ldots,r\}\\
69
+ |\sigma|=p}} B_{j-p}e_\sigma,
70
+ \]
71
+ where $e_\sigma$ has degree $p$. Its homology satisfies
72
+ \[
73
+ \dim_F H_p(K_\bullet(B)_j)=\beta^A_{p,j}(B).
74
+ \]
75
+ \end{lemma}
76
+
77
+ \begin{proof}
78
+ For $\sigma=\{i_1<\cdots<i_p\}$ the differential is
79
+ \[
80
+ d(be_\sigma)=\sum_{q=1}^p(-1)^{q-1}y_{i_q}b\,
81
+ e_{\sigma\setminus\{i_q\}}.
82
+ \]
83
+ The complex $K_\bullet(A)$ is the tensor product over $F$ of the
84
+ one-variable complexes
85
+ \[
86
+ 0\longrightarrow F[y_i](-1)
87
+ \xrightarrow{\ y_i\ }F[y_i]\longrightarrow0.
88
+ \]
89
+ Each has homology $F$ in position zero and no other homology. A complex
90
+ of vector spaces splits as its homology with zero differential plus
91
+ contractible two-term summands. Tensoring these splittings shows that
92
+ $K_\bullet(A)$ is a free resolution of $F$.
93
+
94
+ To compare this computation with a resolution of $B$, take any graded
95
+ free resolution $F_\bullet\to B$ and form the first-quadrant double
96
+ complex $F_\bullet\otimes_A K_\bullet(A)$. Augmenting either factor
97
+ gives maps from its total complex to $F_\bullet\otimes_A F$ and to
98
+ $B\otimes_A K_\bullet(A)$, respectively. The kernels have exact columns
99
+ or exact rows, since the terms of the other factor are free. Their
100
+ total complexes are exact. For exact columns, eliminate a cycle's
101
+ component of greatest horizontal index by a vertical boundary; the
102
+ correction introduces terms only in the next column to the left.
103
+ There are finitely many components on each total-degree diagonal,
104
+ so iteration eliminates the cycle. The argument for exact rows
105
+ interchanges the two indices. Both augmentation maps consequently induce
106
+ homology isomorphisms. This identifies the homology of
107
+ $B\otimes_A K_\bullet(A)=K_\bullet(B)$ with $\Tor^A(B,F)$, preserving
108
+ the internal grading.
109
+ \end{proof}
110
+
111
+ We now order monomial positions without choosing an order on their
112
+ coefficients. Let $V$ be a finite-dimensional $F$-vector space in
113
+ degree zero, and set
114
+ \[
115
+ E=V\otimes_F A=\bigoplus_{\alpha\in\Z_{\geq0}^r}Vy^\alpha.
116
+ \]
117
+ Choose a total order $\prec$ on the exponents of each fixed total
118
+ degree, compatible with addition: if $\alpha\prec\beta$, then
119
+ $\alpha+\gamma\prec\beta+\gamma$ for every
120
+ $\gamma\in\Z_{\geq0}^r$. The first nonzero position of an element is
121
+ its leading position in this order.
122
+
123
+ For a homogeneous submodule $W\subseteq E$ and an exponent $\alpha$,
124
+ define
125
+ \[
126
+ V_\alpha=\left\{v\in V:
127
+ vy^\alpha+\sum_{\substack{|\gamma|=|\alpha|\\\alpha\prec\gamma}}
128
+ v_\gamma y^\gamma\in W
129
+ \text{ for some }v_\gamma\in V\right\}.
130
+ \]
131
+ This is an $F$-subspace of $V$. The resulting leading submodule is
132
+ \[
133
+ \operatorname{in}_{\prec}W
134
+ =\bigoplus_{\alpha\in\Z_{\geq0}^r}V_\alpha y^\alpha.
135
+ \]
136
+ Indeed, multiplication of a witnessing element by $y_i$ shows that
137
+ $V_\alpha\subseteq V_{\alpha+e_i}$, so this direct sum is an
138
+ $A$-submodule.
139
+
140
+ \begin{proposition}[Leading-submodule comparison]
141
+ \label{filt:comparison}
142
+ \label{filt:initial}
143
+ With $A,V,E,W$ and $\prec$ as above, for every $d\in\Z$, every
144
+ $p\geq0$, and every $j\in\Z$ one has
145
+ \begin{align}
146
+ \dim_F(E/W)_d
147
+ &=\dim_F(E/\operatorname{in}_{\prec}W)_d,
148
+ \label{filt:hilbert}\\
149
+ \beta^A_{p,j}(E/W)
150
+ &\leq\beta^A_{p,j}(E/\operatorname{in}_{\prec}W).
151
+ \label{filt:betti}
152
+ \end{align}
153
+ \end{proposition}
154
+
155
+ \begin{proof}
156
+ Write $Q=E/W$. In degree $d\geq0$, let $E_{\succeq\alpha}$ be the
157
+ sum of the positions $Vy^\gamma$ with $|\gamma|=d$ and
158
+ $\alpha\preceq\gamma$, and define $E_{\succ\alpha}$ similarly with
159
+ strict inequality. Their images in $Q_d$ give a finite descending
160
+ filtration. Its quotient at $\alpha$ is
161
+ \begin{equation}
162
+ \frac{\operatorname{im}(E_{\succeq\alpha}\to Q_d)}
163
+ {\operatorname{im}(E_{\succ\alpha}\to Q_d)}
164
+ \simeq
165
+ \frac{E_{\succeq\alpha}}
166
+ {E_{\succ\alpha}+(W_d\cap E_{\succeq\alpha})}
167
+ \simeq (V/V_\alpha)y^\alpha.
168
+ \label{filt:slot-quotient}
169
+ \end{equation}
170
+ The last isomorphism takes the coefficient at $\alpha$. Summing its
171
+ dimensions proves \eqref{filt:hilbert}; both sides vanish for $d<0$.
172
+
173
+ Fix an internal degree $j\geq0$. We give all terms of
174
+ $K_\bullet(Q)_j$ a common filtration indexed by the degree-$j$
175
+ exponents. For a subset $\sigma$, put
176
+ $\mathbf{1}_\sigma=\sum_{i\in\sigma}e_i$. In the summand with
177
+ exterior label $e_\sigma$, place the coefficient position $\alpha$ at
178
+ \[
179
+ \alpha+\mathbf{1}_\sigma.
180
+ \]
181
+ More explicitly, the filtration subspace at $\beta$ in that summand
182
+ is the image of the span of all $Vy^\alpha$ satisfying
183
+ $\beta\preceq\alpha+\mathbf{1}_\sigma$. The full filtration subspace
184
+ is the direct sum over the labels $\sigma$. Addition compatibility
185
+ means that the relative order of the positions within one summand
186
+ agrees with their order in $Q_{j-|\sigma|}$.
187
+
188
+ A differential deleting $i\in\sigma$ multiplies its coefficient by
189
+ $y_i$. It sends the position with exponent $\alpha$ to that with
190
+ exponent $\alpha+e_i$, and
191
+ \[
192
+ (\alpha+e_i)+\mathbf{1}_{\sigma\setminus\{i\}}
193
+ =\alpha+\mathbf{1}_\sigma.
194
+ \]
195
+ Thus the differential preserves the filtration. By
196
+ \eqref{filt:slot-quotient}, its map on the corresponding associated
197
+ graded positions is, up to the Koszul sign,
198
+ \[
199
+ V/V_\alpha\longrightarrow V/V_{\alpha+e_i},
200
+ \qquad [v]\longmapsto[v].
201
+ \]
202
+ This is well defined by $V_\alpha\subseteq V_{\alpha+e_i}$.
203
+ Consequently the associated graded complex is exactly
204
+ $K_\bullet(E/\operatorname{in}_{\prec}W)_j$, decomposed by the total
205
+ exponent $\beta$.
206
+
207
+ For completeness, if $d:C\to C'$ is a filtration-preserving linear
208
+ map between finite-dimensional filtered spaces, the filtration induced
209
+ on $\ker d$ gives an injection
210
+ \[
211
+ \operatorname{gr}(\ker d)
212
+ \hookrightarrow\ker(\operatorname{gr}d).
213
+ \]
214
+ Indeed a leading class represented by an element of $\ker d$ maps to
215
+ zero, and the induced filtration on the kernel makes this inclusion
216
+ injective. Since taking associated graded preserves dimension, it
217
+ follows that
218
+ $\operatorname{rank}d\geq\operatorname{rank}(\operatorname{gr}d)$.
219
+ At a fixed term of a complex, the homology dimension is the term
220
+ dimension minus the ranks of its incoming and outgoing maps. Applying
221
+ the rank inequality to these two maps proves that passing to the
222
+ associated graded complex cannot decrease this homology dimension.
223
+ Lemma~\ref{filt:koszul} now gives \eqref{filt:betti}. For $j<0$ all
224
+ the relevant Koszul terms vanish, so the same assertion holds.
225
+ \end{proof}
226
+
227
+ Taking $V=F$ recovers the usual comparison with a monomial initial
228
+ ideal; see also \cite[Section~2]{MM}. Keeping $V$ arbitrary is essential
229
+ for the next application:
230
+ the coefficient algebra will enlarge all dimensions by the same
231
+ finite factor, which can then be cancelled.
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/03-monomial.tex ADDED
@@ -0,0 +1,218 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A monomial bound containing the prescribed powers}
2
+ \label{sec:monomial}
3
+
4
+ We use the commuting forms of Theorem~\ref{thm:forms} to construct a
5
+ monomial ideal containing the prescribed powers. The construction
6
+ preserves the Hilbert function and increases every graded Betti number.
7
+ The first step explains why the original resolution remains minimal
8
+ over the polynomial ring acting through these forms.
9
+
10
+ \begin{lemma}[Transfer of a minimal resolution]
11
+ \label{mono:transfer}
12
+ Let $S=\C[x_1,\ldots,x_n]$, let $k$ be a field containing $\C$, and
13
+ let $\Delta$ be a finite-dimensional central division $k$-algebra.
14
+ Put $m=\dim_k\Delta$ and
15
+ $N=\Delta[x_1,\ldots,x_n]$, where the $x_i$ are central.
16
+ Suppose that $t_1,\ldots,t_n\in N_1$ commute and that
17
+ \begin{equation}
18
+ N=\bigoplus_{\alpha\in\Z_{\geq0}^n}\Delta t^\alpha
19
+ \label{mono:basis}
20
+ \end{equation}
21
+ is a graded direct-sum decomposition. Give
22
+ $T=k[y_1,\ldots,y_n]$ a right action on $N$ by multiplication,
23
+ $u\cdot y_i=ut_i$.
24
+ For every homogeneous ideal $I\subseteq S$, the right $T$-module
25
+ $Q=N/IN$ satisfies
26
+ \begin{align}
27
+ \dim_k Q_d&=m\dim_\C(S/I)_d
28
+ &&(d\in\Z),\label{mono:dimension-transfer}\\
29
+ \beta^T_{p,j}(Q)&=m\beta^S_{p,j}(S/I)
30
+ &&(p\geq0,\ j\in\Z).
31
+ \label{mono:betti-transfer}
32
+ \end{align}
33
+ Here right and left modules over the commutative ring $T$ are
34
+ identified when computing $\Tor$.
35
+ \end{lemma}
36
+
37
+ \begin{proof}
38
+ Commutativity of the $t_i$ and centrality of $k$ make the stated right
39
+ $T$-action well defined. The map
40
+ \begin{equation}
41
+ \Delta\otimes_kT\longrightarrow N,
42
+ \qquad b\otimes y^\alpha\longmapsto bt^\alpha
43
+ \label{mono:free-map}
44
+ \end{equation}
45
+ is a graded vector-space isomorphism by \eqref{mono:basis}. It is
46
+ right $T$-linear because $(bt^\alpha)t_i=bt^{\alpha+e_i}$.
47
+ Thus $N$ is right $T$-free of rank $m$, with a basis in degree zero,
48
+ and
49
+ \begin{equation}
50
+ N_{>0}=NT_{>0}.
51
+ \label{mono:positive-degree}
52
+ \end{equation}
53
+
54
+ The left $S$-action commutes with the right $T$-action by associativity
55
+ of multiplication in $N$. Moreover,
56
+ $N=\Delta\otimes_\C S$ as a left $S$-module, so $N$ is left $S$-free
57
+ and therefore flat. Each element of $I$ is central in $N$, whence
58
+ $IN$ is a two-sided ideal. In particular it is a right $T$-submodule,
59
+ and
60
+ \[
61
+ Q\simeq\Delta\otimes_\C(S/I).
62
+ \]
63
+ Taking a complex basis of $(S/I)_d$ proves
64
+ \eqref{mono:dimension-transfer}.
65
+
66
+ Let $F_\bullet\to S/I$ be a minimal graded $S$-free resolution.
67
+ Since $S$ is commutative, regard its terms as right $S$-modules and
68
+ tensor with the $(S,T)$-bimodule $N$. Flatness gives a resolution
69
+ \[
70
+ F_\bullet\otimes_SN\longrightarrow Q
71
+ \]
72
+ by graded free right $T$-modules. An entry $f$ of an original
73
+ differential acts on $N$ by left multiplication. This map is right
74
+ $T$-linear, again by associativity.
75
+
76
+ Choose a $k$-basis $b_1,\ldots,b_m$ of $\Delta$, which is a right
77
+ $T$-basis of $N$ under \eqref{mono:free-map}. If $f$ is nonzero and
78
+ has degree $e>0$, then each $fb_u$ belongs to $N_e$. By the graded
79
+ decomposition \eqref{mono:basis}, its coefficients in the basis
80
+ $b_1,\ldots,b_m$ are homogeneous polynomials in $T$ of degree $e$.
81
+ They therefore lie in $T_{>0}$. Every nonzero original differential
82
+ entry has positive degree, so the transferred resolution is minimal.
83
+ Each summand $S(-s)$ of $F_p$ becomes $m$ summands $T(-s)$.
84
+ Lemma~\ref{filt:minimal} proves \eqref{mono:betti-transfer} for every
85
+ $p,j$. If $I=S$, both quotients and their resolutions may be taken
86
+ to be zero, and the same formulas hold.
87
+ \end{proof}
88
+
89
+ The next proposition supplies the monomial ideal used by the rest of
90
+ the proof. Its ideal is allowed to depend on $I$, but it is fixed
91
+ simultaneously for all homological and internal degrees.
92
+
93
+ \begin{proposition}[Monomial reduction]
94
+ \label{mono:bound}
95
+ Let $S=\C[x_1,\ldots,x_n]$, let
96
+ $2\leq a_1\leq\cdots\leq a_n$, and let $I\subseteq S$ be a
97
+ homogeneous ideal containing a homogeneous regular sequence
98
+ $f_1,\ldots,f_n$ with $\deg f_h=a_h$. Put
99
+ $P=(x_1^{a_1},\ldots,x_n^{a_n})$.
100
+ There is a monomial ideal $M\subseteq S$ containing $P$ such that
101
+ \begin{align}
102
+ \dim_\C(S/M)_d&=\dim_\C(S/I)_d
103
+ &&(d\in\Z),\label{mono:hilbert-bound}\\
104
+ \beta^S_{p,j}(S/I)&\leq\beta^S_{p,j}(S/M)
105
+ &&(p\geq0,\ j\in\Z).
106
+ \label{mono:betti-bound}
107
+ \end{align}
108
+ \end{proposition}
109
+
110
+ \begin{proof}
111
+ If $I=S$, take $M=S$. Assume henceforth that $I$ is proper.
112
+ Apply Theorem~\ref{thm:forms} to the given regular sequence. It
113
+ supplies $k$, $\Delta$, and commuting degree-one forms $t_h$ satisfying
114
+ the basis property \eqref{mono:basis} and homogeneous identities
115
+ \begin{equation}
116
+ t_h^{a_h}=c_hf_h+\sum_{\ell<h}B_{h\ell}f_\ell
117
+ +\sum_{\ell>h}C_{h\ell}t_\ell,
118
+ \qquad c_h\in k^\times,
119
+ \label{mono:triangular}
120
+ \end{equation}
121
+ where the multipliers belong to $N=\Delta[x_1,\ldots,x_n]$.
122
+ In particular $C_{h\ell}$ is homogeneous of degree $a_h-1$ when
123
+ nonzero. Define $T=k[y_1,\ldots,y_n]$, $m=\dim_k\Delta$,
124
+ $W=IN$, and $Q=N/W$ as in Lemma~\ref{mono:transfer}.
125
+
126
+ Under \eqref{mono:free-map}, view $N$ as the free $T$-module with
127
+ coefficient space $V=\Delta$. In each total degree, order exponents
128
+ by placing the lexicographically smallest tuple
129
+ \[
130
+ (\alpha_n,\ldots,\alpha_1)
131
+ \]
132
+ first. This order is compatible with addition. Apply
133
+ Proposition~\ref{filt:comparison} to the homogeneous $T$-submodule
134
+ $W$ with this order.
135
+
136
+ For an exponent $\alpha$, let $V_\alpha\subseteq\Delta$ be its
137
+ leading coefficient space. It is closed under left multiplication
138
+ by $\Delta$: if $w\in W$ witnesses a coefficient $b$ at $\alpha$
139
+ with no earlier coefficients, then $\lambda w\in W$ witnesses
140
+ $\lambda b$. Here $W$ is left $\Delta$-linear because it is an ideal
141
+ of $N$. Hence $V_\alpha$ is a left ideal of $\Delta$. Since
142
+ $\Delta$ is a division algebra,
143
+ \[
144
+ V_\alpha=0\quad\hbox{or}\quad\Delta.
145
+ \]
146
+ Explicitly, if $0\ne b\in V_\alpha$, every $c\in\Delta$ is
147
+ $(cb^{-1})b$ and therefore also belongs to $V_\alpha$.
148
+
149
+ The set
150
+ \[
151
+ \mathcal U=\{\alpha\in\Z_{\geq0}^n:V_\alpha=\Delta\}
152
+ \]
153
+ is upward closed under addition of exponent vectors, since the leading
154
+ object is a $T$-submodule. Define $M\subseteq S$ to be the monomial
155
+ ideal with exponent set $\mathcal U$, and define
156
+ $M_k\subseteq T$ by the same exponent set. Then
157
+ \begin{equation}
158
+ N/\operatorname{in}_{\prec}W
159
+ \simeq\Delta\otimes_k(T/M_k)
160
+ \simeq(T/M_k)^{\oplus m}
161
+ \label{mono:initial-quotient}
162
+ \end{equation}
163
+ as graded right $T$-modules.
164
+
165
+ We next verify the power containment. Since every $f_\ell$ lies
166
+ in $I$, Equation~\eqref{mono:triangular} gives
167
+ \[
168
+ t_h^{a_h}-\sum_{\ell>h}C_{h\ell}t_\ell\in W.
169
+ \]
170
+ Expand each $C_{h\ell}$ in the left $\Delta$-basis $t^\alpha$.
171
+ Right multiplication by $t_\ell$ turns a term $bt^\alpha$ into
172
+ $bt^{\alpha+e_\ell}$, using only commutativity of the forms.
173
+ Every resulting exponent has a positive coordinate of index greater
174
+ than $h$. It consequently lies strictly after $a_he_h$ in the
175
+ chosen order, because $a_he_h$ has zero coordinates at all indices
176
+ greater than $h$. The displayed element therefore has leading
177
+ position $a_he_h$ with coefficient $1$. Thus $a_he_h\in\mathcal U$
178
+ for every $h$, proving $P\subseteq M$.
179
+
180
+ It remains to compare the numerical invariants. The scalar extension
181
+ of $S/M$ from $\C$ to $k$, with $x_i$ renamed $y_i$, is $T/M_k$.
182
+ Its Hilbert function is unchanged. Tensoring the Koszul complex over
183
+ $\C$ with the field $k$ also preserves exactness and commutes with
184
+ homology, so
185
+ \begin{align*}
186
+ \dim_k(T/M_k)_d&=\dim_\C(S/M)_d,\\
187
+ \beta^T_{p,j}(T/M_k)&=\beta^S_{p,j}(S/M).
188
+ \end{align*}
189
+ Equations \eqref{mono:dimension-transfer} and
190
+ \eqref{mono:initial-quotient}, together with
191
+ \eqref{filt:hilbert}, now give
192
+ \[
193
+ m\dim_\C(S/I)_d
194
+ =\dim_k Q_d
195
+ =\dim_k(N/\operatorname{in}_{\prec}W)_d
196
+ =m\dim_\C(S/M)_d.
197
+ \]
198
+ Likewise, \eqref{mono:betti-transfer},
199
+ \eqref{filt:betti}, and \eqref{mono:initial-quotient} yield, for
200
+ every $p\geq0$ and every $j\in\Z$,
201
+ \[
202
+ m\beta^S_{p,j}(S/I)
203
+ =\beta^T_{p,j}(Q)
204
+ \leq\beta^T_{p,j}(N/\operatorname{in}_{\prec}W)
205
+ =m\beta^S_{p,j}(S/M).
206
+ \]
207
+ Cancelling the positive integer $m$ proves both assertions.
208
+ \end{proof}
209
+
210
+ The right action in Lemma~\ref{mono:transfer} and the placement of the
211
+ $\Delta$-coefficients on the left are deliberate. The argument uses
212
+ commutativity among the forms $t_i$, but never requires an individual
213
+ coefficient in $\Delta$ to commute with a form. Proposition~\ref{mono:bound}
214
+ completes the reduction to an ideal containing $P$. The remaining
215
+ comparison is the prescribed-powers theorem of Mermin and Murai
216
+ \cite[Theorem~3.1]{MM}. Sections~\ref{sec:stabilization}--\ref{sec:tor}
217
+ give a direct proof by stabilization, box compression, and a Koszul-rank
218
+ induction.
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/04-stabilization.tex ADDED
@@ -0,0 +1,216 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Stabilization inside the exponent box}
2
+ \label{sec:stabilization}
3
+
4
+ We now start with a monomial ideal containing the prescribed powers.
5
+ The aim of this section is to impose stability inside the finite exponent
6
+ box while preserving the Hilbert function and weakly increasing every
7
+ graded Betti number of the quotient. This is the pure-power
8
+ deformation strategy of Mermin and Murai \cite[Section~3]{MM}.
9
+
10
+ Let
11
+ \[
12
+ S=\C[x_1,\ldots,x_n],\qquad
13
+ 2\le a_1\le\cdots\le a_n,\qquad
14
+ P=(x_1^{a_1},\ldots,x_n^{a_n}),\qquad b_i=a_i-1.
15
+ \]
16
+ For $1\le r\le n$ and $d\in\Z$, put
17
+ \[
18
+ \mathcal B_r(d)
19
+ =\{u\in\Z_{\ge0}^r: |u|=d,\ 0\le u_i\le b_i
20
+ \text{ for }1\le i\le r\}.
21
+ \]
22
+ In particular, this set is empty when $d<0$.
23
+
24
+ \begin{definition}
25
+ \label{stab:definition}
26
+ A subset $X\subseteq\mathcal B_r(d)$ is \emph{stable} if
27
+ \[
28
+ u\in X,\quad h<\ell,\quad
29
+ u+e_h-e_\ell\in\mathcal B_r(d)
30
+ \quad\Longrightarrow\quad u+e_h-e_\ell\in X.
31
+ \]
32
+ A monomial ideal containing $(x_1^{a_1},\ldots,x_r^{a_r})$ is
33
+ \emph{stable in the box} if its included exponent vectors in
34
+ $\mathcal B_r(d)$ form a stable set for every $d$.
35
+ This definition imposes no transfer condition on monomials outside the box.
36
+ \end{definition}
37
+
38
+ The modification used below acts on one pair of variables. Fix
39
+ $h<\ell$, write $\xi=x_h$ and $q=x_\ell$, and choose a primitive
40
+ $a_\ell$-th root of unity $\zeta\in\C$. Define a graded
41
+ $\C$-linear map $D:S\to S$ on monomials by
42
+ \begin{equation}
43
+ \label{stab:distraction-formula}
44
+ D(x^u)=\left(\prod_{i\ne\ell}x_i^{u_i}\right)
45
+ \prod_{s=0}^{u_\ell-1}(q-\zeta^s\xi),
46
+ \qquad u\in\Z_{\ge0}^n,
47
+ \end{equation}
48
+ with the empty product equal to $1$.
49
+ The resolution argument below is the nested-factor mechanism used for
50
+ distractions in~\cite[Theorem~2.19 and Corollary~2.20]{BCR}.
51
+ We give the argument directly because the
52
+ root-of-unity factors here are periodic, rather than eventually constant.
53
+
54
+ \begin{lemma}
55
+ \label{stab:distraction}
56
+ For every monomial ideal $K\subseteq S$, its vector-space image $D(K)$
57
+ is a homogeneous ideal. Moreover,
58
+ \begin{gather*}
59
+ \dim_\C(S/D(K))_d=\dim_\C(S/K)_d
60
+ \quad(d\in\Z),\\
61
+ \beta^S_{p,j}(S/D(K))=\beta^S_{p,j}(S/K)
62
+ \quad(p\ge0,\ j\in\Z).
63
+ \end{gather*}
64
+ The map also satisfies $D(P)=P$.
65
+ \end{lemma}
66
+
67
+ \begin{proof}
68
+ The expansion of $D(x^u)$ has coefficient $1$ at $x^u$, and every
69
+ other monomial is lexicographically larger than $x^u$. Thus $D$ is
70
+ unitriangular on each finite-dimensional graded piece and is invertible.
71
+ Multiplication by a variable other than $q$ commutes with $D$, while
72
+ \begin{equation}
73
+ \label{stab:multiplication}
74
+ qD(x^u)=D(qx^u)+\zeta^{u_\ell}\xi D(x^u).
75
+ \end{equation}
76
+ Since $K$ is spanned by monomials and is an ideal, these identities show
77
+ that $D(K)$ is an ideal. The invertibility and degree preservation of
78
+ $D$ give the Hilbert-function equality.
79
+
80
+ To check preservation of $P$, first observe that
81
+ \[
82
+ \prod_{s=0}^{a_\ell-1}(q-\zeta^s\xi)
83
+ =q^{a_\ell}-\xi^{a_\ell}\in P.
84
+ \]
85
+ Here the second term belongs to $P$ because $a_h\le a_\ell$.
86
+ If a monomial is divisible by $q^{a_\ell}$, its image under $D$ is
87
+ divisible by this displayed polynomial. If it is divisible by another
88
+ generator of $P$, that generator remains a factor of its image.
89
+ Consequently $D(P)\subseteq P$. In each degree this inclusion is an
90
+ inclusion between vector spaces of the same finite dimension, so it is
91
+ an equality.
92
+
93
+ It remains to compare Betti numbers. If $K=S$, both quotients are zero.
94
+ Otherwise, choose a minimal exponent-multigraded free resolution
95
+ $F_\bullet\to S/K$ with $F_0=S$, as in
96
+ Lemma~\ref{filt:minimal}. A nonzero differential entry from a generator
97
+ of multidegree $u$ to one of multidegree $v$ has the form
98
+ $c x^{u-v}$, where $u\ge v$ coordinatewise. Keeping the ordinary
99
+ graded free modules, replace this entry by
100
+ \begin{equation}
101
+ \label{stab:ratio-entry}
102
+ c\frac{D(x^u)}{D(x^v)}.
103
+ \end{equation}
104
+ The ratio is a polynomial: all unchanged monomial factors are nested,
105
+ as are the products in~\eqref{stab:distraction-formula}.
106
+
107
+ For each free summand whose generator has multidegree $v$, define a
108
+ linear change on its coefficient polynomials by
109
+ \begin{equation}
110
+ \label{stab:coefficient-change}
111
+ C_v(x^{w-v})=\frac{D(x^w)}{D(x^v)},\qquad w\ge v.
112
+ \end{equation}
113
+ More explicitly, the right-hand side is
114
+ \[
115
+ \left(\prod_{i\ne\ell}x_i^{w_i-v_i}\right)
116
+ \prod_{s=v_\ell}^{w_\ell-1}(q-\zeta^s\xi).
117
+ \]
118
+ It has the original monomial $x^{w-v}$ with coefficient $1$ and only
119
+ lexicographically larger additional terms. Hence $C_v$ is an
120
+ invertible graded vector-space map. These maps need not be
121
+ $S$-linear; the new differential defined by~\eqref{stab:ratio-entry}
122
+ is $S$-linear.
123
+
124
+ The changes on the free summands intertwine the old and new
125
+ differentials. Indeed, for a source coefficient $x^{w-u}$ and a
126
+ nonzero entry $c x^{u-v}$, the required equality is precisely
127
+ \[
128
+ \frac{D(x^w)}{D(x^u)}
129
+ \left(c\frac{D(x^u)}{D(x^v)}\right)
130
+ =c\frac{D(x^w)}{D(x^v)}.
131
+ \]
132
+ Thus the new maps form a complex that is exact in every positive
133
+ homological degree. At $F_0=S$ the change is $C_0=D$, so its image
134
+ from $F_1$ is $D(K)$. We have obtained a free resolution of $S/D(K)$
135
+ with the same ordinary graded free modules as $F_\bullet$.
136
+ Every replaced nonzero entry still has its original positive degree,
137
+ so this resolution is minimal. Its free ranks in each degree give
138
+ the asserted equality of all graded Betti numbers.
139
+ \end{proof}
140
+
141
+ \begin{proposition}
142
+ \label{stab:main}
143
+ Let $S=\C[x_1,\ldots,x_n]$, let $2\le a_1\le\cdots\le a_n$,
144
+ and put $P=(x_1^{a_1},\ldots,x_n^{a_n})$.
145
+ For every monomial ideal $K\supseteq P$, there is a monomial ideal
146
+ $H\supseteq P$ stable in the box such that
147
+ \[
148
+ \dim_\C(S/H)_d=\dim_\C(S/K)_d\quad(d\in\Z)
149
+ \]
150
+ and
151
+ \[
152
+ \beta^S_{p,j}(S/K)\le\beta^S_{p,j}(S/H)
153
+ \qquad(p\ge0,\ j\in\Z).
154
+ \]
155
+ \end{proposition}
156
+
157
+ \begin{proof}
158
+ If $K$ is stable in the box, take $H=K$. Otherwise choose a failed
159
+ transfer from $q=x_\ell$ to $\xi=x_h$, with $h<\ell$, and form
160
+ the map $D$ above. Replace $K$ by
161
+ \[
162
+ K'=\operatorname{in}_{\mathrm{lex}}D(K),
163
+ \]
164
+ where the leading monomial is the lexicographically largest one.
165
+ By Lemma~\ref{stab:distraction}, $P\subseteq D(K)$, and hence
166
+ $P\subseteq K'$. That lemma and Proposition~\ref{filt:comparison}
167
+ show that the Hilbert function is preserved and
168
+ \[
169
+ \beta^S_{p,j}(S/K)\le\beta^S_{p,j}(S/K')
170
+ \qquad(p\ge0,\ j\in\Z).
171
+ \]
172
+ We prove that repeated replacements terminate by measuring progress
173
+ in every lexicographic prefix.
174
+
175
+ Fix a degree $d$ and a prefix $E$ of the degree-$d$ monomials, listed
176
+ from greatest to least. Let $\pi_E$ be the projection onto their span.
177
+ Gaussian elimination with this ordered list of columns gives
178
+ \[
179
+ \#\{m\in E:m\in K'\}
180
+ =\dim_\C\pi_E(D(K)_d).
181
+ \]
182
+ For the monomials $m\in K\cap E$, the vectors $\pi_E(D(m))$
183
+ are linearly independent: their coordinates in their original
184
+ monomial positions form a triangular matrix with diagonal entries $1$.
185
+ Consequently
186
+ \begin{equation}
187
+ \label{stab:prefix-growth}
188
+ \#(K'\cap E)\ge\#(K\cap E)
189
+ \end{equation}
190
+ for every such prefix in every degree.
191
+
192
+ There is a strict inequality for at least one prefix. Choose a
193
+ monomial $x^u\in K$ inside the box witnessing the failed transfer, so
194
+ \[
195
+ m'=\frac{\xi}{q}x^u
196
+ \quad\text{lies inside the box but does not belong to }K.
197
+ \]
198
+ Its existence implies $1\le u_\ell<a_\ell$. Let $E$ be the
199
+ degree-$|u|$ prefix ending at $m'$. Every monomial in $K\cap E$
200
+ is strictly larger than $m'$, so its $D$-image has zero coefficient
201
+ at $m'$. On the other hand, the coefficient at $m'$ of $D(x^u)$ is
202
+ \[
203
+ -\sum_{s=0}^{u_\ell-1}\zeta^s
204
+ =-\frac{1-\zeta^{u_\ell}}{1-\zeta}\ne0.
205
+ \]
206
+ Thus $\pi_E(D(x^u))$ is independent of the projected vectors already
207
+ used for $K\cap E$, proving strictness in~\eqref{stab:prefix-growth}.
208
+
209
+ Every monomial ideal containing $P$ is determined by the monomials
210
+ it includes in the finite box $0\le u_i<a_i$. There are therefore
211
+ only finitely many such ideals. The nondecreasing prefix counts,
212
+ with at least one strict increase at every replacement, prevent a
213
+ repetition. Continuing whenever stability fails must consequently
214
+ stop at an ideal $H$ stable in the box. The Hilbert-function equalities
215
+ and all Betti inequalities persist along this finite sequence.
216
+ \end{proof}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/05-boxes.tex ADDED
@@ -0,0 +1,269 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Shadows and end slices in an exponent box}
2
+ \label{sec:boxes}
3
+
4
+ We now replace the monomials of a stable ideal, degree by degree, by
5
+ lex segments in the exponent box. The shadow comparison below will
6
+ ensure that the replacement is an ideal. At the same time we prove
7
+ two comparisons for its first and last slices.
8
+ The bounded-monomial theorem of Clements and Lindstr\"om gives the shadow
9
+ comparison for arbitrary subsets when the bounds are nondecreasing
10
+ \cite{CL}. Here we assume stability of the subsets, allow the bounds in
11
+ arbitrary order, and prove the two endpoint comparisons together with
12
+ the shadow inequality.
13
+
14
+ Recall the notation for a box with positive integer bounds
15
+ \(b_1,\ldots,b_r\):
16
+ \[
17
+ \mathcal B_r(d)=
18
+ \left\{u\in\Z_{\ge0}^{\,r}:
19
+ \sum_{h=1}^r u_h=d,\quad u_h\le b_h\text{ for every }h\right\}.
20
+ \]
21
+ Here \(d\) may be any integer; in particular the box is empty when
22
+ \(d<0\) or \(d>\sum_h b_h\). We also set
23
+ \(\mathcal B_0(0)=\{()\}\) and \(\mathcal B_0(d)=\varnothing\) for
24
+ \(d\ne0\). No ordering of the bounds is required in this section.
25
+
26
+ Vectors are ordered lexicographically, with the first coordinate
27
+ taking precedence, and lex segments start with the largest vectors.
28
+ For \(X\subseteq\mathcal B_r(d)\), let
29
+ \(\operatorname{Lex}(X)\) be the lex segment of cardinality \(|X|\).
30
+ Recall that \(X\) is \emph{stable} if
31
+ \[
32
+ u\in X,\quad h<\ell,\quad
33
+ u+e_h-e_\ell\in\mathcal B_r(d)
34
+ \quad\Longrightarrow\quad u+e_h-e_\ell\in X.
35
+ \]
36
+ Every lex segment is stable, since each allowed transfer increases
37
+ the vector in lex order. Define the bounded shadow and the slices by
38
+ \[
39
+ \begin{split}
40
+ \partial X
41
+ &=\{u+e_h\in\mathcal B_r(d+1):u\in X,\ 1\le h\le r\},\\
42
+ X(s)
43
+ &=\{u\in\mathcal B_{r-1}(d-s):(u,s)\in X\}
44
+ \qquad(0\le s\le b_r).
45
+ \end{split}
46
+ \]
47
+ The bounds in \(\mathcal B_{r-1}\) are the first \(r-1\) bounds.
48
+ Empty sets have empty shadows; thus these definitions also cover
49
+ negative degrees and empty slices.
50
+
51
+ \begin{lemma}[Shadows and end slices]
52
+ \label{box:inequalities}
53
+ Let \(r\ge1\), let \(b_1,\ldots,b_r\) be positive integers, and let
54
+ \(d\in\Z\). If \(X\subseteq\mathcal B_r(d)\) is stable and
55
+ \(Y=\operatorname{Lex}(X)\), then \(\partial Y\) is a lex segment and
56
+ \begin{equation}
57
+ \label{box:three-inequalities}
58
+ |\partial X|\ge|\partial Y|,
59
+ \qquad |X(0)|\ge|Y(0)|,
60
+ \qquad |X(b_r)|\le|Y(b_r)|.
61
+ \end{equation}
62
+ \end{lemma}
63
+
64
+ \begin{proof}
65
+ We first prove the assertion about lex shadows, without assuming
66
+ stability of \(X\). Empty shadows need no argument. For
67
+ \(v\in\mathcal B_r(d+1)\), with \(d\ge0\), its lex largest
68
+ degree-\(d\) predecessor is
69
+ \[
70
+ p(v)=v-e_{\max\{h:v_h>0\}}.
71
+ \]
72
+ Every predecessor belongs to the bounded box. Moreover, the map
73
+ \(p\) preserves weak lex order. Indeed, suppose \(v>w\), with first
74
+ difference at coordinate \(k\). Subtraction at the last nonzero
75
+ coordinate cannot change an earlier coordinate of \(v\). If the
76
+ operation changes a coordinate of \(w\) before \(k\), then
77
+ \(p(v)>p(w)\) already at that coordinate. Otherwise the strict
78
+ inequality at \(k\) can disappear only if \(v_k=w_k+1\) and the tail
79
+ of \(v\) after \(k\) is zero. Equality of total degrees then says
80
+ that the tail of \(w\) contains exactly one unit. Subtracting its
81
+ last nonzero coordinate gives \(p(v)=p(w)\). In all other cases the
82
+ first strict inequality remains. Membership of \(v\) in the shadow
83
+ of a lex segment is equivalent to membership of \(p(v)\) in that
84
+ segment, proving that its shadow is lex.
85
+
86
+ We prove the three inequalities simultaneously by induction on
87
+ \(r\). If \(\mathcal B_r(d)\) is empty, they are immediate. For
88
+ \(r=1\), each degree box has at most one vector, so \(X=Y\).
89
+ Assume henceforth that \(r>1\). A prime will indicate lex
90
+ replacement or shadow in the first \(r-1\) coordinates.
91
+
92
+ Each slice \(X(s)\) is stable, and stability between slices gives
93
+ \begin{equation}
94
+ \label{box:original-slices}
95
+ \partial'X(s)\subseteq X(s-1)
96
+ \qquad(1\le s\le b_r).
97
+ \end{equation}
98
+ Replace each slice by \(Z(s)=\operatorname{Lex}'(X(s))\), and let
99
+ \(Z\subseteq\mathcal B_r(d)\) be the set with these slices.
100
+ By the induction hypothesis and \eqref{box:original-slices},
101
+ \[
102
+ |\partial'Z(s)|\le|\partial'X(s)|\le|X(s-1)|=|Z(s-1)|.
103
+ \]
104
+ The shadow on the left and the slice on the right are lex segments
105
+ in the same degree box. Consequently
106
+ \begin{equation}
107
+ \label{box:compressed-slices}
108
+ \partial'Z(s)\subseteq Z(s-1)
109
+ \qquad(1\le s\le b_r).
110
+ \end{equation}
111
+ Thus a unit in the last coordinate of a member of \(Z\) may be moved
112
+ to any earlier coordinate with available capacity, while remaining
113
+ in \(Z\).
114
+
115
+ \smallskip\noindent
116
+ \emph{The zero slice.}
117
+ If \(Z(0)=\mathcal B_{r-1}(d)\), then
118
+ \(|Y(0)|\le|Z(0)|=|X(0)|\). Otherwise let \(v\) be the largest
119
+ vector of \(\mathcal B_{r-1}(d)\) omitted from \(Z(0)\); all members
120
+ of \(Z(0)\) are strictly larger than \(v\).
121
+
122
+ We claim that every \((u,s)\in Z\) is strictly larger than
123
+ \((v,0)\). Equality is excluded by the choice of \(v\). If instead
124
+ \((u,s)<(v,0)\), let \(k<r\) be their first differing coordinate.
125
+ Then \(u_k<v_k\) and earlier coordinates agree. Also \(s>0\),
126
+ since every member of the lex slice \(Z(0)\) is larger than \(v\).
127
+ We will
128
+ move the \(s\) units of the last coordinate into the first \(r-1\)
129
+ coordinates to obtain a vector \(w\le v\).
130
+
131
+ Let
132
+ \[
133
+ c=\sum_{k<j<r}(b_j-u_j)
134
+ \]
135
+ be the available capacity strictly after coordinate \(k\). If
136
+ \(s\le c\), distribute all \(s\) units among those positions; the
137
+ result still has \(w_k=u_k<v_k\). If \(s>c\), fill all those
138
+ positions and put the remaining \(s-c\) units at coordinate \(k\).
139
+ Since \(|u|+s=|v|=d\) and the prefixes before \(k\) agree,
140
+ \begin{equation}
141
+ \label{box:tail-filling}
142
+ s-c
143
+ =v_k-u_k-\sum_{k<j<r}(b_j-v_j)
144
+ \le v_k-u_k.
145
+ \end{equation}
146
+ The remaining units therefore fit at \(k\). If the inequality in
147
+ \eqref{box:tail-filling} is strict, then \(w_k<v_k\). If equality
148
+ holds, every coordinate of the tail of \(v\) is full, and the
149
+ constructed vector is exactly \(v\). In either case \(w\le v\).
150
+ All the moves stay within the bounds, so repeated use of
151
+ \eqref{box:compressed-slices} gives \(w\in Z(0)\), a contradiction.
152
+ This proves the claim.
153
+
154
+ There are thus at least \(|Z|=|X|\) vectors preceding \((v,0)\).
155
+ The lex segment \(Y\) of that cardinality also consists entirely of
156
+ vectors preceding \((v,0)\). Its zero slice is therefore contained
157
+ in \(Z(0)\), proving
158
+ \begin{equation}
159
+ \label{box:zero-slice}
160
+ |Y(0)|\le|Z(0)|=|X(0)|.
161
+ \end{equation}
162
+
163
+ \smallskip\noindent
164
+ \emph{The top slice.}
165
+ Put \(B=\sum_{h=1}^r b_h\) and let
166
+ \(\rho(u)=(b_1-u_1,\ldots,b_r-u_r)\). The reflected complement
167
+ \[
168
+ X^*=\rho\bigl(\mathcal B_r(d)\setminus X\bigr)
169
+ \subseteq\mathcal B_r(B-d)
170
+ \]
171
+ is stable. In fact, if an allowed upward transfer took a member
172
+ of \(X^*\) outside \(X^*\), reflection would give an upward transfer
173
+ from a member of \(X\) to a vector outside \(X\), contradicting
174
+ stability. Reflection reverses lex order, so
175
+ \(Y^*=\rho(\mathcal B_r(d)\setminus Y)\) is the lex segment of
176
+ cardinality \(|X^*|\).
177
+
178
+ The zero-slice inequality, already proved in \(r\) coordinates,
179
+ applies to \(X^*,Y^*\). Their zero-slice cardinalities are
180
+ \[
181
+ \begin{split}
182
+ |X^*(0)|&=|\mathcal B_{r-1}(d-b_r)|-|X(b_r)|,\\
183
+ |Y^*(0)|&=|\mathcal B_{r-1}(d-b_r)|-|Y(b_r)|.
184
+ \end{split}
185
+ \]
186
+ It follows that \(|X(b_r)|\le|Y(b_r)|\).
187
+
188
+ \smallskip\noindent
189
+ \emph{The shadow.}
190
+ We have established both end-slice comparisons. To recover the
191
+ shadow bound, we separate its zero slice from the remaining vectors.
192
+ For any stable set \(X\),
193
+ \begin{equation}
194
+ \label{box:shadow-count}
195
+ |\partial X|=|\partial'X(0)|+|X|-|X(b_r)|.
196
+ \end{equation}
197
+ Indeed, its shadow vectors with last coordinate zero are precisely
198
+ \(\partial'X(0)\). Every shadow vector \(v\) with positive last
199
+ coordinate has \(v-e_r\in X\): if it was obtained as \(v=u+e_h\)
200
+ with \(h<r\), transfer one unit of the positive last coordinate of
201
+ \(u\) to coordinate \(h\). This transfer is within bounds because
202
+ \(v\) is within bounds. Stability gives \(v-e_r\in X\).
203
+ Thus adding \(e_r\) bijects the members of \(X\) outside its top
204
+ slice with shadow vectors having positive last coordinate,
205
+ proving~\eqref{box:shadow-count}.
206
+
207
+ The same identity holds for the stable set \(Y\). Its zero slice
208
+ is a lex segment, and \eqref{box:zero-slice} gives
209
+ \(Y(0)\subseteq\operatorname{Lex}'(X(0))\). The induction
210
+ hypothesis and monotonicity of shadows under inclusion imply
211
+ \[
212
+ |\partial'X(0)|
213
+ \ge\bigl|\partial'\operatorname{Lex}'(X(0))\bigr|
214
+ \ge|\partial'Y(0)|.
215
+ \]
216
+ Combining this with the top-slice inequality in
217
+ \eqref{box:shadow-count} proves \(|\partial X|\ge|\partial Y|\)
218
+ and completes the induction.
219
+ \end{proof}
220
+
221
+ We apply the shadow comparison to the degree pieces of a monomial
222
+ ideal. For \(A=\C[x_1,\ldots,x_r]\) and
223
+ \(P_r=(x_1^{b_1+1},\ldots,x_r^{b_r+1})\), a monomial ideal
224
+ \(H\supseteq P_r\) is stable in the box sense precisely when each
225
+ set
226
+ \[
227
+ X_d=\{u\in\mathcal B_r(d):x^u\in H\}
228
+ \]
229
+ is stable. Define its degreewise lex replacement by
230
+ \begin{equation}
231
+ \label{box:lex-replacement}
232
+ (\Lambda H)_d
233
+ =(P_r)_d+
234
+ \operatorname{span}_{\C}
235
+ \{x^u:u\in\operatorname{Lex}(X_d)\},
236
+ \qquad
237
+ \Lambda H=\bigoplus_{d\ge0}(\Lambda H)_d.
238
+ \end{equation}
239
+ At this point \(\Lambda H\) is a graded vector subspace; the next
240
+ proposition verifies its closure under multiplication.
241
+
242
+ \begin{proposition}[Lex replacement is an ideal]
243
+ \label{box:ideal}
244
+ Let \(b_1,\ldots,b_r\) be positive integers, and let
245
+ \(H\subseteq\C[x_1,\ldots,x_r]\) be a monomial ideal containing
246
+ \(P_r=(x_1^{b_1+1},\ldots,x_r^{b_r+1})\) and stable in the box
247
+ sense. Then the subspace \(\Lambda H\) defined in
248
+ \eqref{box:lex-replacement} is a monomial ideal containing \(P_r\).
249
+ It is stable in the box sense and has the same Hilbert function as
250
+ \(H\).
251
+ \end{proposition}
252
+
253
+ \begin{proof}
254
+ Write \(Y_d=\operatorname{Lex}(X_d)\). Since \(H\) is an ideal,
255
+ \(\partial X_d\subseteq X_{d+1}\). Lemma~\ref{box:inequalities}
256
+ therefore gives
257
+ \[
258
+ |\partial Y_d|\le|\partial X_d|
259
+ \le|X_{d+1}|=|Y_{d+1}|.
260
+ \]
261
+ Both \(\partial Y_d\) and \(Y_{d+1}\) are lex segments in
262
+ \(\mathcal B_r(d+1)\), so \(\partial Y_d\subseteq Y_{d+1}\).
263
+ Thus multiplying a monomial of \(\Lambda H\) by a variable either
264
+ gives a monomial of the next lex segment or leaves the box and
265
+ enters \(P_r\). Products of monomials already in \(P_r\) stay in
266
+ \(P_r\). This proves the ideal assertion. Each \(Y_d\) is stable
267
+ and has cardinality \(|X_d|\), which proves stability and equality
268
+ of Hilbert functions.
269
+ \end{proof}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/06-tor.tex ADDED
@@ -0,0 +1,256 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Betti bounds for stable ideals}
2
+ \label{sec:tor}
3
+
4
+ The preceding section shows that degreewise lex replacement of a
5
+ monomial ideal stable in the box is again an ideal with the same
6
+ Hilbert function. We prove that this replacement also bounds every
7
+ graded Betti number. The induction on the number of variables uses
8
+ the first and last box slices. After reduction modulo the last variable,
9
+ these determine two endpoint modules; the middle modules have zero
10
+ Koszul differentials.
11
+
12
+ For modules with the same Hilbert function, the Koszul terms have equal
13
+ dimensions in every homological and internal degree. An upper bound on
14
+ Betti numbers is therefore equivalent to a lower bound on the sum of the
15
+ two adjacent differential ranks. We first isolate this rank sum, which
16
+ does not increase under taking either submodules or quotients.
17
+ Let $m\ge0$ and $R=\C[x_1,\ldots,x_m]$. For a graded $R$-module $B$ with
18
+ finite-dimensional graded pieces, write $K^R_\bullet(B)$ for its
19
+ Koszul complex and define its \emph{Koszul rank deficit} by
20
+ \begin{equation}
21
+ \label{tor:deficit-definition}
22
+ D^R_{p,j}(B)=\dim_\C K^R_p(B)_j-\beta^R_{p,j}(B),
23
+ \qquad p\ge0,\quad j\in\Z.
24
+ \end{equation}
25
+ Terms of the Koszul complex outside its homological range are zero.
26
+
27
+ \begin{lemma}
28
+ \label{tor:deficit}
29
+ For every $p\ge0$ and $j\in\Z$, the quantity $D^R_{p,j}(B)$
30
+ is the sum of the ranks of the two Koszul differentials adjacent to
31
+ $K^R_p(B)_j$. If $U\subseteq B$ is a graded submodule and $V$ is
32
+ a graded quotient of $B$, then
33
+ \[
34
+ D^R_{p,j}(U)\le D^R_{p,j}(B),\qquad
35
+ D^R_{p,j}(V)\le D^R_{p,j}(B).
36
+ \]
37
+ The quantity is additive on finite direct sums, satisfies
38
+ \[
39
+ D^R_{p,j}(B(-s))=D^R_{p,j-s}(B),
40
+ \]
41
+ and vanishes when $R_{>0}B=0$.
42
+ \end{lemma}
43
+
44
+ \begin{proof}
45
+ Write $d_p(B)_j:K^R_p(B)_j\to K^R_{p-1}(B)_j$ for the Koszul
46
+ differential. Since its homology computes $\Tor^R(B,\C)$,
47
+ \[
48
+ \beta^R_{p,j}(B)
49
+ =\dim_\C K^R_p(B)_j
50
+ -\operatorname{rank}d_p(B)_j
51
+ -\operatorname{rank}d_{p+1}(B)_j.
52
+ \]
53
+ This proves the rank formula. The Koszul complex of $U$ embeds
54
+ termwise into that of $B$, and the image of each of its differentials
55
+ embeds into the corresponding differential image for $B$.
56
+ For the quotient $V$, the termwise surjections give
57
+ \[
58
+ \operatorname{im}d_p(V)_j
59
+ =\text{the image of }\operatorname{im}d_p(B)_j
60
+ \text{ in }K^R_{p-1}(V)_j.
61
+ \]
62
+ Thus each of the two ranks can only decrease under either operation.
63
+ Direct sums and grading shifts commute with the Koszul complex.
64
+ Finally, if all the variables annihilate $B$, every Koszul differential
65
+ is zero.
66
+ \end{proof}
67
+
68
+ \begin{theorem}
69
+ \label{tor:stable}
70
+ Let $r\ge1$, let $2\le a_1\le\cdots\le a_r$, and let
71
+ $A=\C[x_1,\ldots,x_r]$. Suppose that $H\subseteq A$ is a
72
+ monomial ideal containing $(x_1^{a_1},\ldots,x_r^{a_r})$ and is
73
+ stable in the box. Let $G=\Lambda H$ be its degreewise lex
74
+ replacement inside the box, together with the prescribed pure powers.
75
+ Then, for every $p\ge0$ and $j\in\Z$,
76
+ \[
77
+ \beta^A_{p,j}(H)\le\beta^A_{p,j}(G),
78
+ \qquad
79
+ \beta^A_{p,j}(A/H)\le\beta^A_{p,j}(A/G).
80
+ \]
81
+ \end{theorem}
82
+
83
+ \begin{proof}
84
+ By Proposition~\ref{box:ideal}, $G$ is an ideal stable in the box
85
+ and has the same Hilbert function as $H$. If $H=A$, then $G=A$
86
+ and both comparisons are equalities. For proper $H$, the ideal
87
+ comparison implies the quotient comparison in positive homological
88
+ degrees by Lemma~\ref{filt:minimal}:
89
+ \begin{equation}
90
+ \label{tor:ideal-quotient}
91
+ \beta^A_{p+1,j}(A/H)=\beta^A_{p,j}(H),
92
+ \qquad
93
+ \beta^A_{p+1,j}(A/G)=\beta^A_{p,j}(G).
94
+ \end{equation}
95
+ The two quotient Betti numbers in homological degree zero are both
96
+ $1$ when $j=0$ and $0$ otherwise. We prove the two comparisons
97
+ simultaneously by induction on $r$, establishing the ideal comparison
98
+ and then using~\eqref{tor:ideal-quotient}. When $r=1$, a monomial
99
+ ideal containing $x_1^{a_1}$ is a power ideal or the full ring, and
100
+ $H=G$.
101
+
102
+ Assume $r>1$ and $H$ proper, and put
103
+ \[
104
+ R=\C[x_1,\ldots,x_{r-1}],\qquad z=x_r,\qquad a=a_r.
105
+ \]
106
+ For $s\ge0$, define coefficient ideals
107
+ \[
108
+ H^{(s)}=\{u\in R:uz^s\in H\},\qquad
109
+ G^{(s)}=\{u\in R:uz^s\in G\}.
110
+ \]
111
+ These are ascending monomial ideals containing the earlier prescribed
112
+ powers, and they equal $R$ for $s\ge a$. For $s<a$, their
113
+ stability in the earlier-variable box follows by applying stability
114
+ with the last exponent fixed at $s$. For $1\le s<a$ we also have
115
+ \begin{equation}
116
+ \label{tor:slice-annihilation}
117
+ R_{>0}H^{(s)}\subseteq H^{(s-1)},\qquad
118
+ R_{>0}G^{(s)}\subseteq G^{(s-1)}.
119
+ \end{equation}
120
+ To see the first inclusion, it is enough to multiply a monomial of
121
+ $H^{(s)}$ by an earlier variable $x_i$. If its earlier-variable
122
+ exponent, or that exponent after multiplication by $x_i$, is outside
123
+ the box, the earlier powers already imply the required membership.
124
+ Otherwise stability moves one factor of $z$ to $x_i$. The proof
125
+ for $G$ is identical.
126
+
127
+ We next pass from ideals over $A$ to modules over $R$. Multiplication
128
+ by $z$ is injective on $H$, since $H$ is an ideal in the domain $A$.
129
+ Set
130
+ \[
131
+ B_H=H/zH,\qquad B_G=G/zG.
132
+ \]
133
+ Reducing a minimal $A$-free resolution of $H$ modulo $z$ gives a
134
+ minimal $R$-free resolution of $B_H$. Here is a direct exactness
135
+ check. Lift a cycle in positive homological degree modulo $z$ to
136
+ an element $y$ of the free resolution, and write $dy=zv$.
137
+ Applying the next differential shows that $v$ is a cycle, using
138
+ injectivity of $z$ on the free modules; in degree zero, apply the
139
+ augmentation and use injectivity of $z$ on $H$ instead.
140
+ Exactness gives $v=du$, so $y-zu$ is a cycle and hence a boundary.
141
+ Its reduction modulo $z$ is the original cycle. Right exactness
142
+ identifies the cokernel with $B_H$, and all differential entries
143
+ remain of positive degree or become zero, so minimality is preserved.
144
+ The same argument applies to $G$. Therefore
145
+ \begin{equation}
146
+ \label{tor:reduction}
147
+ \beta^A_{p,j}(H)=\beta^R_{p,j}(B_H),\qquad
148
+ \beta^A_{p,j}(G)=\beta^R_{p,j}(B_G).
149
+ \end{equation}
150
+ The injective multiplication maps also give
151
+ \[
152
+ \dim_\C(B_H)_d=\dim_\C H_d-\dim_\C H_{d-1},\qquad
153
+ \dim_\C(B_G)_d=\dim_\C G_d-\dim_\C G_{d-1}.
154
+ \]
155
+ Consequently $B_H$ and $B_G$ have equal Hilbert functions.
156
+
157
+ The monomial decomposition by powers of $z$ describes these modules
158
+ more precisely; this is the decomposition appearing in
159
+ \cite[Lemma~3.7]{CS}. The coefficient of $z^0$ in $H/zH$ is $H^{(0)}$,
160
+ and its coefficient of $z^s$ for $s\ge1$ is
161
+ $H^{(s)}/H^{(s-1)}$. Since $H^{(s)}=R$ for $s\ge a$, this gives
162
+ an isomorphism of graded $R$-modules
163
+ \begin{equation}
164
+ \label{tor:slice-decomposition}
165
+ B_H\cong H^{(0)}
166
+ \oplus\bigoplus_{s=1}^{a-1}
167
+ (H^{(s)}/H^{(s-1)})(-s)
168
+ \oplus(R/H^{(a-1)})(-a).
169
+ \end{equation}
170
+ There are no terms for $s>a$. The shifts record that multiplication
171
+ by $z^s$ raises ordinary degree by $s$. By
172
+ \eqref{tor:slice-annihilation}, all middle summands are annihilated
173
+ by the variables of $R$, as illustrated in
174
+ Figure~\ref{fig:endpoint-slices}. The decomposition is $R$-linear
175
+ because multiplying by an earlier variable preserves the exponent of
176
+ $z$. The middle summands still contribute to $\Tor$, but their
177
+ Koszul differentials have rank zero. Thus they contribute nothing to
178
+ the deficits. Lemma~\ref{tor:deficit} yields
179
+ \begin{equation}
180
+ \label{tor:endpoint-deficits}
181
+ D^R_{p,j}(B_H)
182
+ =D^R_{p,j}(H^{(0)})
183
+ +D^R_{p,j-a}(R/H^{(a-1)}),
184
+ \end{equation}
185
+ and the identical formula holds for $G$.
186
+
187
+ \input{figures/endpoint-slices}
188
+
189
+ It remains to compare the two endpoint contributions. Write
190
+ $\Lambda'$ for lex replacement with the earlier prescribed powers
191
+ in $R$. The induction hypothesis applies to both $H^{(0)}$ and
192
+ $H^{(a-1)}$. It gives an ideal comparison for the first and a
193
+ quotient comparison for the second. Their respective lex
194
+ replacements have the same Hilbert functions, and hence the same
195
+ Koszul term dimensions. Subtracting the Betti inequalities from
196
+ these dimensions gives
197
+ \begin{align}
198
+ D^R_{p,j}(H^{(0)})
199
+ &\ge D^R_{p,j}(\Lambda'H^{(0)}),
200
+ \label{tor:induction-zero}\\
201
+ D^R_{p,j-a}(R/H^{(a-1)})
202
+ &\ge D^R_{p,j-a}(R/\Lambda'H^{(a-1)}).
203
+ \label{tor:induction-top}
204
+ \end{align}
205
+ This also covers any coefficient ideal equal to $R$: its lex
206
+ replacement is $R$, the corresponding ideal comparison is equality,
207
+ and its quotient is zero.
208
+
209
+ The slice inequalities of Lemma~\ref{box:inequalities} imply
210
+ \begin{equation}
211
+ \label{tor:endpoint-inclusions}
212
+ G^{(0)}\subseteq\Lambda'H^{(0)},\qquad
213
+ \Lambda'H^{(a-1)}\subseteq G^{(a-1)}.
214
+ \end{equation}
215
+ Indeed, fix an earlier-variable degree $e\ge0$. For the first
216
+ inclusion, apply the zero-slice inequality to the included exponent
217
+ sets of $H$ and $G$ in total degree $e$. For the second, apply
218
+ the top-slice inequality in total degree $e+a-1$. Each slice of
219
+ $G$ is already a lex segment in the earlier-variable box, so its
220
+ cardinality comparison with the corresponding slice of $H$ becomes
221
+ the stated containment in the appropriate lex replacement.
222
+ All monomials outside the earlier-variable box belong to both ideals.
223
+ This proves the inclusions in every degree.
224
+
225
+ Apply Lemma~\ref{tor:deficit} to the first inclusion in
226
+ \eqref{tor:endpoint-inclusions} and to the quotient map furnished
227
+ by the second:
228
+ \[
229
+ R/\Lambda'H^{(a-1)}\longrightarrow R/G^{(a-1)}.
230
+ \]
231
+ Together with~\eqref{tor:induction-zero} and
232
+ \eqref{tor:induction-top}, this gives
233
+ \begin{align*}
234
+ D^R_{p,j}(H^{(0)})&\ge D^R_{p,j}(G^{(0)}),\\
235
+ D^R_{p,j-a}(R/H^{(a-1)})
236
+ &\ge D^R_{p,j-a}(R/G^{(a-1)}).
237
+ \end{align*}
238
+ Adding and using~\eqref{tor:endpoint-deficits}, we obtain
239
+ \[
240
+ D^R_{p,j}(B_H)\ge D^R_{p,j}(B_G).
241
+ \]
242
+ The equal Hilbert functions of $B_H$ and $B_G$ imply
243
+ \[
244
+ \dim_\C K^R_p(B_H)_j
245
+ =\binom{r-1}{p}\dim_\C(B_H)_{j-p}
246
+ =\dim_\C K^R_p(B_G)_j,
247
+ \]
248
+ with the binomial coefficient interpreted as zero outside its range.
249
+ Subtracting the deficit inequality from these equal dimensions gives
250
+ $\beta^R_{p,j}(B_H)\le\beta^R_{p,j}(B_G)$.
251
+ Equation~\eqref{tor:reduction} proves the ideal comparison over $A$,
252
+ and~\eqref{tor:ideal-quotient} completes the quotient comparison.
253
+ Every step applies to every $p\ge0$ and $j\in\Z$; in particular,
254
+ negative internal degrees and Koszul terms outside their homological
255
+ range introduce no additional cases.
256
+ \end{proof}
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/07-assembly.tex ADDED
@@ -0,0 +1,53 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{The prescribed lex-plus-powers ideal}\label{sec:assembly}
2
+
3
+ We now combine the comparisons, keeping the same ideal at every
4
+ homological and internal degree.
5
+
6
+ \begin{proof}[Proof of Theorem~\ref{thm:main}]
7
+ If \(I=S\), then \(L_d=S_d\) is allowed in every degree and \(J=S\);
8
+ all quotient Betti numbers are zero. Assume \(I\ne S\).
9
+ Proposition~\ref{mono:bound} gives a monomial ideal \(M\supseteq P\)
10
+ with the Hilbert function of \(I\) and
11
+ \[
12
+ \beta^S_{p,j}(S/I)\le\beta^S_{p,j}(S/M)
13
+ \qquad(p\ge0,\ j\in\Z).
14
+ \]
15
+ Proposition~\ref{stab:main} gives a box-stable monomial ideal
16
+ \(H\supseteq P\), with the same Hilbert function, and
17
+ \[
18
+ \beta^S_{p,j}(S/M)\le\beta^S_{p,j}(S/H).
19
+ \]
20
+ By Proposition~\ref{box:ideal}, the degreewise box-lex replacement
21
+ \(G=\Lambda H\) is an ideal, with the same Hilbert function.
22
+ Theorem~\ref{tor:stable} gives
23
+ \[
24
+ \beta^S_{p,j}(S/H)\le\beta^S_{p,j}(S/G).
25
+ \]
26
+
27
+ It remains to check that \(G\) is the ideal prescribed in
28
+ \eqref{eq:prescription}.
29
+ In degree \(d\), list all monomials in decreasing lex order and remove
30
+ those belonging to \(P_d\). The remaining list is exactly
31
+ \(\mathcal B_n(d)\) in decreasing lex order.
32
+ The monomials of \(G_d\) outside \(P_d\) are the first
33
+ \[
34
+ q_d=\dim_\C I_d-\dim_\C P_d
35
+ \]
36
+ positions of this remaining list. This integer lies between zero and
37
+ \(|\mathcal B_n(d)|\), because \(H\supseteq P\) has the same Hilbert
38
+ function as \(I\).
39
+
40
+ Every box prefix is obtained by intersecting some full-list prefix with
41
+ the box. Thus a lex-segment subspace \(L_d\) with
42
+ \(\dim_\C(L_d+P_d)=\dim_\C I_d\) exists. Enlarging that full-list prefix
43
+ to the largest one of the same resulting dimension adds only monomials
44
+ already in \(P_d\), and does not change the sum. Consequently
45
+ \(L_d+P_d=G_d\) for every \(d\), including the empty and full box cases.
46
+ Hence \(J=G\). The displayed comparisons prove all the asserted Betti
47
+ bounds for this single \(J\).
48
+ \end{proof}
49
+
50
+ The argument proves idealness and all syzygy bounds together.
51
+ The use of \(\C\) enters the commuting-form construction and supplies the
52
+ roots of unity for stabilization; no conclusion in positive
53
+ characteristic is asserted for an arbitrary regular sequence.
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/build/sections/08-characteristic-zero.tex ADDED
@@ -0,0 +1,85 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Arbitrary regular-sequence length and characteristic-zero fields}
2
+ \label{sec:characteristic-zero}
3
+
4
+ The new input of this paper is the Artinian theorem over \(\C\). We now
5
+ apply the published Artinian reduction and record the coefficient-field
6
+ argument needed for Corollary~\ref{cor:characteristic-zero}.
7
+
8
+ \begin{proof}[Proof of Corollary~\ref{cor:characteristic-zero}]
9
+ If \(I=S_F\), the prescription gives \(J=S_F\), and all quotient Betti
10
+ numbers vanish. We may therefore assume that \(I\) is proper.
11
+
12
+ First let \(F=\C\). After a linear change of coordinates, one may arrange
13
+ that
14
+ \[
15
+ f_1,\ldots,f_c,x_{c+1},\ldots,x_n
16
+ \]
17
+ is a regular sequence; the list of variables is empty when \(c=n\).
18
+ Write \(\overline f_i\) for the images of the \(f_i\) in
19
+ \(\overline S=\C[x_1,\ldots,x_c]\). They form a full regular sequence
20
+ of degrees \(a_1,\ldots,a_c\). Theorem~\ref{thm:main}, applied in
21
+ \(\overline S\) to every homogeneous ideal containing this sequence,
22
+ gives both the Eisenbud--Green--Harris and lex-plus-powers assertions for
23
+ \(\overline f_1,\ldots,\overline f_c\).
24
+
25
+ The Artinian reduction of Caviglia--Maclagan
26
+ \cite[Proposition~10]{CM08} transfers the Hilbert-function assertion to
27
+ \(f_1,\ldots,f_c\). Theorem~4.1 of Caviglia--Kummini \cite{CK14}
28
+ transfers the Betti assertion as well. Their formulation uses Betti
29
+ numbers of ideals. For any proper homogeneous ideal \(K\) in a standard
30
+ graded polynomial ring \(A\), the exact sequence
31
+ \(0\to K\to A\to A/K\to0\) gives
32
+ \[
33
+ \beta^A_{p+1,j}(A/K)=\beta^A_{p,j}(K)
34
+ \qquad(p\ge0,\ j\in\Z).
35
+ \]
36
+ The remaining quotient Betti number is \(\beta^A_{0,0}(A/K)=1\).
37
+ Thus their convention is equivalent to the quotient convention used
38
+ here. The lexicographic embedding modulo \(P_F\) in that reduction
39
+ selects exactly the prescribed \(q_d\) greatest monomials outside \(P_F\)
40
+ in each degree. A linear change of coordinates preserves Hilbert functions
41
+ and graded Betti numbers, so this proves the corollary over \(\C\).
42
+
43
+ Now let \(F\) be any characteristic-zero field. Choose homogeneous
44
+ generators \(g_1,\ldots,g_r\) of \(I\), and let \(F_0\subseteq F\) be
45
+ the field generated over \(\Q\) by all coefficients of the \(g_i\) and
46
+ the \(f_i\). Set
47
+ \[
48
+ S_0=F_0[x_1,\ldots,x_n],\qquad
49
+ I_0=(g_1,\ldots,g_r,f_1,\ldots,f_c)\subseteq S_0.
50
+ \]
51
+ Then \(I_0S_F=I\). The sequence \(f_1,\ldots,f_c\) is regular in
52
+ \(S_0\): after tensoring each multiplication map with the faithfully
53
+ flat extension \(F/F_0\), it is the corresponding injective map over
54
+ \(S_F\). The finitely generated characteristic-zero field \(F_0\)
55
+ admits an embedding into \(\C\). Extending by this embedding preserves
56
+ regularity, so the case just proved applies to
57
+ \[
58
+ S_{\C}=\C\otimes_{F_0}S_0,\qquad I_{\C}=I_0S_{\C}.
59
+ \]
60
+ No embedding of \(F\) into \(\C\) is needed.
61
+
62
+ Let \(J_{\C}\) be the resulting lex-plus-powers ideal. It is a monomial
63
+ ideal, so let \(J_0\subseteq S_0\) be generated by the same monomials and
64
+ put \(J_F=J_0S_F\). For \(E=F\) or \(E=\C\), let
65
+ \(S_E=E\otimes_{F_0}S_0\). Graded field base change preserves the
66
+ dimensions of homogeneous pieces. It also gives, for \(M_0=S_0/I_0\)
67
+ and for \(M_0=S_0/J_0\),
68
+ \[
69
+ E\otimes_{F_0}\Tor^{S_0}_p(M_0,F_0)_j
70
+ \;\cong\;
71
+ \Tor^{S_E}_p(E\otimes_{F_0}M_0,E)_j.
72
+ \]
73
+ For example, this follows by tensoring the Koszul complex of the
74
+ variables with \(E\); its graded homology commutes with this flat
75
+ extension. Consequently the Hilbert equalities and Betti inequalities
76
+ over \(\C\) give the same equalities and inequalities over \(F\).
77
+ Finally, the monomials of \(P_F\) and the lexicographic order are
78
+ determined by their exponents, while the dimensions defining \(q_d\)
79
+ are unchanged by these field extensions. Hence \(J_F\) is precisely
80
+ the degreewise ideal \(J\) prescribed in the corollary.
81
+ \end{proof}
82
+
83
+ The argument changes the coefficient field only through extensions of
84
+ the common characteristic-zero field \(F_0\). It makes no assertion for
85
+ arbitrary regular sequences in positive characteristic.
preprints/The-Artinian-Lex-Plus-Powers-Betti-Theorem-September-23-2026/paper.pdf ADDED
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+ size 447798
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [The Bass trace conjecture and the characteristic-zero Kaplansky idempotent conjecture](The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** September 24, 2026
6
+
7
+ ## Citation
8
+
9
+ ```bibtex
10
+ @misc{OAI:The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026,
11
+ author = {{OpenAI}},
12
+ title = {{The Bass trace conjecture and the characteristic-zero Kaplansky idempotent conjecture}},
13
+ howpublished = {OpenAI Math Release preprint
14
+ \href{https://github.com/openai/math/blob/main/preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026.pdf}{OAI:The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026}},
15
+ year = {2026}
16
+ }
17
+ ```
18
+
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026.pdf ADDED
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+ oid sha256:1c4d90b5ed4de2ef66b4b07b3d5c3e2bfe8822a538177c64ee1d3c3e091120bf
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+ size 457936
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/main.tex ADDED
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1
+ \documentclass[11pt]{article}
2
+ \usepackage[T1]{fontenc}
3
+ \usepackage{lmodern}
4
+ \usepackage[margin=1.05in]{geometry}
5
+ \usepackage{amsmath,amssymb,amsthm,mathtools}
6
+ \usepackage{microtype,enumitem,booktabs}
7
+ \usepackage{tikz}
8
+ \usetikzlibrary{arrows.meta,positioning}
9
+ \usepackage[colorlinks=true,linkcolor=blue!45!black,citecolor=blue!45!black,urlcolor=blue!45!black]{hyperref}
10
+ \usepackage[nameinlink,noabbrev]{cleveref}
11
+ \newtheorem{theorem}{Theorem}[section]
12
+ \newtheorem{lemma}[theorem]{Lemma}
13
+ \newtheorem{proposition}[theorem]{Proposition}
14
+ \newtheorem{corollary}[theorem]{Corollary}
15
+ \theoremstyle{definition}
16
+ \newtheorem{definition}[theorem]{Definition}
17
+ \theoremstyle{remark}
18
+ \newtheorem{remark}[theorem]{Remark}
19
+ \newcommand{\C}{\mathbb C}
20
+ \newcommand{\R}{\mathbb R}
21
+ \newcommand{\Z}{\mathbb Z}
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+ \newcommand{\N}{\mathbb N}
23
+ \DeclareMathOperator{\HS}{HS}
24
+ \DeclareMathOperator{\HH}{HH}
25
+ \DeclareMathOperator{\tr}{tr}
26
+ \DeclareMathOperator{\supp}{supp}
27
+ \DeclareMathOperator{\con}{con}
28
+ \DeclareMathOperator{\id}{id}
29
+ \numberwithin{equation}{section}
30
+ \setlist{itemsep=3pt,topsep=5pt}
31
+ \setlength{\emergencystretch}{1.5em}
32
+ \pdfinfoomitdate=1
33
+ \pdftrailerid{}
34
+ \pdfsuppressptexinfo=15
35
+ \hypersetup{pdftitle={The Bass trace conjecture and the characteristic-zero Kaplansky idempotent conjecture},pdfauthor={OpenAI}}
36
+ \title{The Bass trace conjecture and the characteristic-zero Kaplansky idempotent conjecture}
37
+ \author{OpenAI}
38
+ \date{September 24, 2026}
39
+ \begin{document}
40
+ \maketitle
41
+ \begin{abstract}
42
+ We prove the complex group-ring Bass trace conjecture for every discrete
43
+ group: the Hattori--Stallings trace of a finitely generated projective module
44
+ over its complex group ring is supported on conjugacy classes of finite-order
45
+ elements. As a consequence, for every torsion-free group $G$ and every
46
+ commutative unital domain $R$ of characteristic zero, the only idempotents
47
+ in $RG$ are $0$ and $1$. This proves Kaplansky's idempotent conjecture in
48
+ characteristic zero.
49
+ \end{abstract}
50
+ \tableofcontents
51
+ \input{sections/01-introduction}
52
+ \input{sections/02-framework}
53
+ \input{sections/03-metric}
54
+ \input{sections/04-filtrations}
55
+ \input{sections/05-surgery}
56
+ \input{sections/06-chains}
57
+ \input{sections/07-idempotents}
58
+ \input{sections/08-detector}
59
+ \input{sections/09-completion}
60
+ \input{sections/10-torsion-free}
61
+ \bibliographystyle{plain}
62
+ \bibliography{references}
63
+ \end{document}
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/references.bib ADDED
@@ -0,0 +1,267 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ @article{Bass1976,
2
+ author = {Bass, Hyman},
3
+ title = {{Euler} characteristics and characters of discrete groups},
4
+ journal = {Inventiones Mathematicae},
5
+ volume = {35},
6
+ year = {1976},
7
+ pages = {155--196},
8
+ doi = {10.1007/BF01390137}
9
+ }
10
+
11
+ @incollection{Bass1979,
12
+ author = {Bass, Hyman},
13
+ title = {Traces and {Euler} characteristics},
14
+ editor = {Wall, C. T. C.},
15
+ booktitle = {Homological Group Theory},
16
+ series = {London Mathematical Society Lecture Note Series},
17
+ volume = {36},
18
+ publisher = {Cambridge University Press},
19
+ address = {Cambridge},
20
+ year = {1979},
21
+ pages = {1--26},
22
+ doi = {10.1017/CBO9781107325449.003}
23
+ }
24
+
25
+ @article{Hattori1965,
26
+ author = {Hattori, Akira},
27
+ title = {Rank element of a projective module},
28
+ journal = {Nagoya Mathematical Journal},
29
+ volume = {25},
30
+ year = {1965},
31
+ pages = {113--120},
32
+ doi = {10.1017/S002776300001148X}
33
+ }
34
+
35
+ @article{Stallings1965,
36
+ author = {Stallings, John},
37
+ title = {Centerless groups---an algebraic formulation of {Gottlieb}'s theorem},
38
+ journal = {Topology},
39
+ volume = {4},
40
+ number = {2},
41
+ year = {1965},
42
+ pages = {129--134},
43
+ doi = {10.1016/0040-9383(65)90060-1}
44
+ }
45
+
46
+ @article{BCM2004,
47
+ author = {Berrick, A. J. and Chatterji, Indira and Mislin, Guido},
48
+ title = {From acyclic groups to the {Bass} conjecture for amenable groups},
49
+ journal = {Mathematische Annalen},
50
+ volume = {329},
51
+ number = {4},
52
+ pages = {597--621},
53
+ year = {2004},
54
+ doi = {10.1007/s00208-004-0521-6},
55
+ url = {https://arxiv.org/abs/1004.1941v1}
56
+ }
57
+
58
+ @article{BCM2006,
59
+ author = {Berrick, A. J. and Chatterji, Indira and Mislin, Guido},
60
+ title = {Homotopy idempotents on manifolds and {Bass}' conjectures},
61
+ journal = {Geometry \& Topology Monographs},
62
+ volume = {10},
63
+ year = {2007},
64
+ pages = {41--62},
65
+ doi = {10.2140/gtm.2007.10.41},
66
+ url = {https://arxiv.org/abs/0903.4341v1}
67
+ }
68
+
69
+ @incollection{CM2011,
70
+ author = {Chatterji, Indira and Mislin, Guido},
71
+ title = {{Hattori--Stallings} trace and {Euler} characteristics for groups},
72
+ booktitle = {Geometric and Cohomological Methods in Group Theory},
73
+ editor = {Bridson, Martin R. and Kropholler, Peter H. and Leary, Ian J.},
74
+ series = {London Mathematical Society Lecture Note Series},
75
+ volume = {358},
76
+ pages = {256--271},
77
+ publisher = {Cambridge University Press},
78
+ year = {2009},
79
+ doi = {10.1017/CBO9781139107099.007},
80
+ url = {https://arxiv.org/abs/0910.4419v1}
81
+ }
82
+
83
+ @article{Linnell1983,
84
+ author = {Linnell, P. A.},
85
+ title = {Decomposition of augmentation ideals and relation modules},
86
+ journal = {Proceedings of the London Mathematical Society},
87
+ series = {3},
88
+ volume = {47},
89
+ number = {1},
90
+ year = {1983},
91
+ pages = {83--127},
92
+ doi = {10.1112/plms/s3-47.1.83}
93
+ }
94
+
95
+ @article{BH2015,
96
+ author = {Berrick, A. J. and Hesselholt, Lars},
97
+ title = {Topological {Hochschild} homology and the {Bass} trace conjecture},
98
+ journal = {J. reine angew. Math.},
99
+ volume = {704},
100
+ year = {2015},
101
+ pages = {169--185},
102
+ doi = {10.1515/crelle-2013-0051},
103
+ url = {https://arxiv.org/abs/1305.6438v2}
104
+ }
105
+
106
+ @article{BV1998,
107
+ author = {Burger, Marc and Valette, Alain},
108
+ title = {Idempotents in complex group rings: theorems of {Zalesskii} and {Bass} revisited},
109
+ journal = {Journal of Lie Theory},
110
+ volume = {8},
111
+ number = {2},
112
+ year = {1998},
113
+ pages = {219--228},
114
+ doi = {10.5802/jolt.142},
115
+ url = {https://jolt.centre-mersenne.org/articles/10.5802/jolt.142/}
116
+ }
117
+
118
+ @article{OW2023,
119
+ author = {{\"O}inert, Johan and Wagner, Stefan},
120
+ title = {Complex group rings and group {$C^*$}-algebras of group extensions},
121
+ journal = {Journal of Algebraic Combinatorics},
122
+ volume = {58},
123
+ year = {2023},
124
+ pages = {387--397},
125
+ doi = {10.1007/s10801-022-01183-6}
126
+ }
127
+
128
+ @article{Connes1985,
129
+ author = {Connes, Alain},
130
+ title = {Non-commutative differential geometry},
131
+ journal = {Publications Math\'ematiques de l'IH\'ES},
132
+ volume = {62},
133
+ year = {1985},
134
+ pages = {41--144},
135
+ doi = {10.1007/BF02698807}
136
+ }
137
+
138
+ @article{Burghelea1985,
139
+ author = {Burghelea, Dan},
140
+ title = {The cyclic homology of the group rings},
141
+ journal = {Commentarii Mathematici Helvetici},
142
+ volume = {60},
143
+ year = {1985},
144
+ pages = {354--365},
145
+ doi = {10.1007/BF02567420}
146
+ }
147
+
148
+ @article{Eckmann1986,
149
+ author = {Eckmann, Beno},
150
+ title = {Cyclic homology of groups and the {Bass} conjecture},
151
+ journal = {Commentarii Mathematici Helvetici},
152
+ volume = {61},
153
+ year = {1986},
154
+ pages = {193--202},
155
+ doi = {10.1007/BF02621911}
156
+ }
157
+
158
+ @misc{Alpert2025,
159
+ author = {Alpert, Hannah},
160
+ title = {Simplicial volume and 0-strata of separating filtrations},
161
+ year = {2024},
162
+ eprint = {2211.06362},
163
+ archivePrefix = {arXiv},
164
+ primaryClass = {math.DG},
165
+ note = {arXiv:2211.06362v3},
166
+ url = {https://arxiv.org/abs/2211.06362v3}
167
+ }
168
+
169
+ @article{Papasoglu2020,
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+ author = {Papasoglu, Panos},
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178
+ }
179
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180
+ @article{BraunSauer2021,
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+ year = {2021},
188
+ doi = {10.1007/s00039-021-00588-y}
189
+ }
190
+
191
+
192
+ @article{Formanek1973,
193
+ author = {Formanek, Edward},
194
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195
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196
+ volume = {25},
197
+ number = {2},
198
+ year = {1973},
199
+ pages = {366--369},
200
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201
+ }
202
+
203
+ @article{FarrellLinnell2003,
204
+ author = {Farrell, F. Thomas and Linnell, Peter A.},
205
+ title = {Whitehead groups and the {Bass} conjecture},
206
+ journal = {Mathematische Annalen},
207
+ volume = {326},
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+ year = {2003},
209
+ pages = {723--757},
210
+ doi = {10.1007/s00208-003-0424-y}
211
+ }
212
+
213
+ @article{BartelsLuckReich2008,
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+ author = {Bartels, Arthur and L{\"u}ck, Wolfgang and Reich, Holger},
215
+ title = {On the {Farrell--Jones} Conjecture and its applications},
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+ }
223
+
224
+ @article{MineyevYu2002,
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+ author = {Mineyev, Igor and Yu, Guoliang},
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+ pages = {97--122},
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233
+ }
234
+
235
+ @article{Puschnigg2002,
236
+ author = {Puschnigg, Michael},
237
+ title = {The {Kadison--Kaplansky} conjecture for word-hyperbolic groups},
238
+ journal = {Inventiones Mathematicae},
239
+ volume = {149},
240
+ number = {1},
241
+ year = {2002},
242
+ pages = {153--194},
243
+ doi = {10.1007/s002220200216}
244
+ }
245
+
246
+ @article{Kantorovich2006,
247
+ author = {Kantorovich, L. V.},
248
+ title = {On the translocation of masses},
249
+ journal = {Journal of Mathematical Sciences},
250
+ volume = {133},
251
+ number = {4},
252
+ year = {2006},
253
+ pages = {1381--1382},
254
+ doi = {10.1007/s10958-006-0049-2},
255
+ note = {Translation of the 1942 original}
256
+ }
257
+
258
+ @article{HjorthMolberg2006,
259
+ author = {Hjorth, Greg and Molberg, Mats},
260
+ title = {Free continuous actions on zero-dimensional spaces},
261
+ journal = {Topology and its Applications},
262
+ volume = {153},
263
+ number = {7},
264
+ year = {2006},
265
+ pages = {1116--1131},
266
+ doi = {10.1016/j.topol.2005.03.003}
267
+ }
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/01-introduction.tex ADDED
@@ -0,0 +1,286 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Introduction}
2
+ \label{sec:introduction}
3
+
4
+ The rank of a projective module over a group ring contains information
5
+ about individual conjugacy classes. This refinement of ordinary rank is
6
+ a basic ingredient of group-ring Euler characteristics: alternating sums
7
+ of projective-module ranks retain information that a numerical Euler
8
+ characteristic forgets \cite{Bass1976,Bass1979}. The Bass trace conjecture
9
+ asks how much of that information can occur at elements of infinite order.
10
+ We first specify the complex version of this question.
11
+
12
+ For a unital complex algebra $A$, let $K_0(A)$ be the Grothendieck group of
13
+ finitely generated projective right $A$-modules, and set
14
+ \[
15
+ \HH_0(A)=A/[A,A],
16
+ \]
17
+ where $[A,A]$ is the complex linear span of commutators. An idempotent
18
+ $e=(e_{ij})\in M_q(A)$ represents the projective right module
19
+ $eA^q$, with matrices acting on columns by left multiplication. Its
20
+ Hattori--Stallings trace is
21
+ \[
22
+ \HS_A([eA^q])=\left[\sum_{i=1}^q e_{ii}\right]\in\HH_0(A),
23
+ \]
24
+ extended additively to virtual projective classes.
25
+
26
+ Let $G$ be a discrete group and write $\con(G)$ for its set of conjugacy
27
+ classes. The quotient $\HH_0(\C G)$ identifies with
28
+ $\bigoplus_{C\in\con(G)}\C C$ by
29
+ \begin{equation}\label{eq:class-trace}
30
+ \left[\sum_{h\in G}a_hh\right]
31
+ \longmapsto
32
+ \sum_{C\in\con(G)}\left(\sum_{h\in C}a_h\right)C.
33
+ \end{equation}
34
+ Indeed, a commutator has zero sum on each conjugacy class, and the
35
+ differences of conjugate group elements span the kernel of the displayed
36
+ map. Such differences are commutators: $tst^{-1}-s=[t,st^{-1}]$.
37
+ All sums arising from an element of $\C G$ have finite support.
38
+ We write $\HS_G(x)(C)$ for the coefficient at $C$.
39
+
40
+ The complex group-ring Bass conjecture asks whether these coefficients
41
+ vanish on every infinite-order conjugacy class, for every group and every
42
+ class in $K_0(\C G)$; see
43
+ \cite[Conjecture 2.1]{BCM2004} and \cite[Conjecture 2]{CM2011}.
44
+
45
+ \begin{theorem}\label{thm:bass}
46
+ Let $G$ be any discrete group. For every $x\in K_0(\C G)$ and every
47
+ infinite-order element $g\in G$,
48
+ \[
49
+ \HS_G(x)([g]_G)=0.
50
+ \]
51
+ Equivalently, if $\con_{\mathrm{fin}}(G)$ denotes the conjugacy classes of
52
+ finite-order elements, then
53
+ \[
54
+ \HS_G\bigl(K_0(\C G)\bigr)
55
+ \subseteq\bigoplus_{C\in\con_{\mathrm{fin}}(G)}\C C.
56
+ \]
57
+ \end{theorem}
58
+
59
+ This resolves the complex group-ring formulation positively. Finite-order
60
+ coefficients need not vanish away from the identity: for a finite group
61
+ $F$, the idempotent $|F|^{-1}\sum_{h\in F}h$ has coefficient
62
+ $|C|/|F|$ at every conjugacy class $C$. The conclusion therefore differs
63
+ from the identity-only support assertion for integral group rings.
64
+ That integral assertion follows in Section~\ref{sec:completion} by combining
65
+ Theorem~\ref{thm:bass} with the known restriction on its finite-order
66
+ coefficients.
67
+
68
+ \subsection{Trace rank and the idempotent conjecture}
69
+
70
+ For a torsion-free group the identity is the only finite-order element,
71
+ so Theorem~\ref{thm:bass} also has numerical and ring-theoretic
72
+ consequences. Define the canonical trace and the augmentation by
73
+ \[
74
+ \tau_G\!\left(\sum_{g\in G}a_g g\right)=a_1,\qquad
75
+ \epsilon_G\!\left(\sum_{g\in G}a_g g\right)=\sum_{g\in G}a_g.
76
+ \]
77
+ For a matrix $b=(b_{ij})\in M_q(\C G)$, put
78
+ $\tau_{G,q}(b)=\sum_{i=1}^q\tau_G(b_{ii})$, and let
79
+ $\epsilon_{G,q}(b)\in M_q(\C)$ be the entrywise augmentation.
80
+ The coefficient at $[1]_G$ of the Hattori--Stallings trace defines
81
+ \[
82
+ \tau_{G,*}:K_0(\C G)\longrightarrow\C,\qquad
83
+ \tau_{G,*}([e(\C G)^q])=\tau_{G,q}(e).
84
+ \]
85
+ The augmentation also defines the integer-valued augmentation rank
86
+ \[
87
+ \operatorname{rk}_{\epsilon}:K_0(\C G)
88
+ \xrightarrow{(\epsilon_G)_*}K_0(\C)
89
+ \xrightarrow{\dim_{\C}}\Z.
90
+ \]
91
+
92
+ The idempotent conjecture commonly attributed to Kaplansky asks whether,
93
+ for every torsion-free group $G$ and every field $k$, an element
94
+ $e\in kG$ satisfying $e^2=e$ must be $0$ or $1$; see
95
+ \cite[Problem 3]{OW2023}. It concerns elements of the group ring itself,
96
+ not arbitrary idempotent matrices over that ring.
97
+
98
+ \begin{corollary}\label{cor:torsion-free}
99
+ Let $G$ be any torsion-free discrete group.
100
+ \begin{enumerate}[label=\textup{(\roman*)}]
101
+ \item For every $q\geq1$ and every idempotent $e\in M_q(\C G)$,
102
+ \[
103
+ \tau_{G,q}(e)=\operatorname{rank}_{\C}\bigl(\epsilon_{G,q}(e)\bigr).
104
+ \]
105
+ Consequently $\tau_{G,*}=\operatorname{rk}_{\epsilon}$, with
106
+ $\Z$ viewed as a subgroup of $\C$, and
107
+ \[
108
+ \tau_{G,*}\bigl(K_0(\C G)\bigr)=\Z.
109
+ \]
110
+ \item For every commutative unital domain $R$ of characteristic zero,
111
+ every $e\in RG$ satisfying $e^2=e$ is either $0$ or $1$.
112
+ \end{enumerate}
113
+ \end{corollary}
114
+
115
+ Part \textup{(ii)} resolves the characteristic-zero Kaplansky idempotent
116
+ conjecture positively, and includes coefficient domains as well as fields.
117
+ Section~\ref{sec:torsion-free} derives both parts from the trace theorem.
118
+ The integer range in part \textup{(i)} concerns algebraic $K_0(\C G)$;
119
+ its relation to the reduced $C^*$-completion is made explicit there.
120
+
121
+ The integral trace consequence also links the theorem to fixed-point
122
+ theory. A map $f$ is a \emph{homotopy idempotent} if $f\circ f\simeq f$.
123
+ Berrick, Chatterji and Mislin's equivalences \cite[Theorems 1--2]{BCM2006}
124
+ then imply that every homotopy idempotent on a connected closed smooth
125
+ oriented manifold of dimension greater than two is freely homotopic to
126
+ a map with exactly one fixed point. They also identify ordinary and
127
+ $L^2$-Lefschetz numbers for pointed homotopy idempotents of connected
128
+ closed smooth oriented manifolds that induce the identity on the
129
+ fundamental group.
130
+ Corollary~\ref{cor:homotopy-idempotents} states these consequences precisely;
131
+ Section~\ref{sec:completion} explains their connection to projective
132
+ Euler characteristics.
133
+
134
+ \subsection{The two parts of the proof}
135
+
136
+ We first describe the algebraic construction to explain the geometric
137
+ statement it needs. The body of the paper begins with that geometric
138
+ statement, formulated independently of group rings, and completes its
139
+ proof before constructing the cycles and cocycles to which it applies.
140
+
141
+ For a finitely generated group $G$, the algebraic construction starts
142
+ with an idempotent $e\in M_q(\C G)$ and one infinite-order element
143
+ $g\in G$. The finitely many nonzero group coefficients of $e$ determine
144
+ a finite set of steps. Products of matrix
145
+ coefficients along paths from $h$ to $gh$, followed by the ordinary
146
+ matrix trace, give complex weights on finite lists of group elements.
147
+ Idempotency says that summing over any intermediate vertex removes that
148
+ vertex. Cyclicity of matrix trace gives a second identity, a cyclic shift
149
+ whose last vertex is multiplied by $g$.
150
+
151
+ Project the vertices to the coset set $Y=\langle g\rangle\backslash G$.
152
+ The group $H=C_G(g)/\langle g\rangle$, where $C_G(g)$ is the centralizer
153
+ of $g$, acts freely on $Y$. For every positive even dimension $2m$, the weighted
154
+ lists define a simplicial cycle modulo this action. Its simplices use
155
+ connected sets of vertices in one graph of bounded degree, fixed as $m$
156
+ increases. A Pfaffian cocycle evaluates on this cycle as
157
+ $2^{-m}\HS_G([e(\C G)^q])([g]_G)$. Here a cocycle means an alternating
158
+ function on vertex lists that vanishes on simplicial boundaries. The
159
+ explicit construction and the evaluation occupy
160
+ Sections~\ref{sec:idempotents} and~\ref{sec:detector}.
161
+
162
+ The geometric part, proved first in Sections~\ref{sec:framework}--\ref{sec:chains},
163
+ shows that every invariant cocycle evaluates to zero on cycles of this
164
+ kind in sufficiently high dimension. We cut the supporting simplicial
165
+ complex successively into pieces of bounded diameter, choosing the
166
+ separating sets nearly to minimize their areas. A volume estimate and
167
+ repeated slicing make the expected number of points in the final
168
+ zero-dimensional set arbitrarily small. A subdivision construction turns
169
+ this point count into a bound for cocycle evaluations. Equivariant chain
170
+ homotopy keeps the evaluation unchanged throughout the construction.
171
+
172
+ The fixed graph degree makes increasing the dimension useful. Through
173
+ each vertex there are only exponentially many connected vertex sets of a
174
+ given size. On an $n$-simplex, Euclidean structures chosen from spanning
175
+ trees of its vertex set give volume $1/n!$; repeated slicing produces the
176
+ same factorial in the comparison with a point of the final separating
177
+ set. After these factors cancel, radii chosen in terms of the fixed
178
+ degree bound make the remaining volume ratio tend to zero with $n$.
179
+ The local replacement argument turns this strict volume margin into the
180
+ small expected point count. No homological-dimension bound on $H$ is
181
+ assumed.
182
+
183
+ Two features permit this argument for arbitrary groups. A compact
184
+ probability space with a free action separates overlapping translates of
185
+ local modifications, without any amenability assumption. Also, each top
186
+ simplex has its own averaged Euclidean area functional. The areas need
187
+ not match along common faces; the successive cuts keep the relevant
188
+ dimensional measures away from those faces.
189
+ The cocycles need not be globally bounded: near each original simplex,
190
+ the construction uses only a fixed finite set of possible vertices.
191
+ Bounding the cocycle on those lists suffices for the evaluation estimate.
192
+
193
+ The final assembly in Section~\ref{sec:completion} chooses a large even
194
+ dimension, forcing the individual trace coefficient to vanish. Passing
195
+ from finitely generated groups to arbitrary groups uses the exact sum
196
+ over subgroup conjugacy classes contained in an ambient conjugacy class.
197
+ Section~\ref{sec:torsion-free} then extracts the augmentation rank from
198
+ the identity coefficient. In the scalar case this rank is $0$ or $1$,
199
+ and the standard faithful-trace argument forces the idempotent itself
200
+ to be $0$ or $1$. A finite-coefficient reduction extends that conclusion
201
+ from complex coefficients to every commutative characteristic-zero domain.
202
+
203
+ \subsection{Relation to previous work}
204
+
205
+ The rank construction comes from Hattori and Stallings
206
+ \cite{Hattori1965,Stallings1965}; Bass developed its relation to Euler
207
+ characteristics and formulated the integral conjecture in
208
+ \cite{Bass1976}; see also \cite[Conjecture (4.5)]{Bass1979}.
209
+ Bass proved complex trace vanishing at infinite-order elements for linear
210
+ groups \cite[Theorem (6.1)(f)]{Bass1979}. For the integral trace,
211
+ Linnell established a restriction on the possible nonzero coefficients
212
+ \cite[Lemma 4.1]{Linnell1983}, later recovered through topological
213
+ Hochschild homology by Berrick and Hesselholt \cite[Theorem A]{BH2015}.
214
+ Its finite-order consequence is the input used in
215
+ Section~\ref{sec:completion}.
216
+
217
+ The scalar idempotent problem also has a long history of trace methods.
218
+ Formanek proved the characteristic-zero conclusion for torsion-free
219
+ groups satisfying the ascending chain condition on subgroups
220
+ \cite[Theorem 1]{Formanek1973}. Burger and Valette revisit the theorems of
221
+ Kaplansky and Zalesskii: the canonical trace of a complex scalar
222
+ idempotent lies in $[0,1]$, its endpoints force the idempotent to be
223
+ trivial, and its value is rational
224
+ \cite[Theorems 1.3 and 2.1]{BV1998}. They also obtain
225
+ $\tau_{G,*}(K_0(\C G))\subseteq\mathbb Q$
226
+ \cite[Corollary 1.2]{BV1998}. Rationality still permits nonintegral
227
+ values strictly between zero and one. For torsion-free groups,
228
+ Theorem~\ref{thm:bass} identifies the trace with augmentation rank,
229
+ which excludes those values. The subsequent faithful-trace argument
230
+ is classical and is included in Section~\ref{sec:torsion-free}.
231
+
232
+ Broader group classes have been treated by algebraic and analytic
233
+ methods. Farrell and Linnell proved the complex Bass statement for
234
+ elementary amenable groups as part of a result over integral domains
235
+ \cite[Theorem 1.6]{FarrellLinnell2003}. Berrick, Chatterji and Mislin
236
+ obtained it for amenable groups through rational surjectivity of the
237
+ degree-zero Bost assembly map for countable groups
238
+ \cite[Theorems 1.3--1.4 and Lemma 1.5]{BCM2004}. Their result concerns
239
+ the stronger trace assertion on $\ell^1(G)$, with finite support on
240
+ finite-order classes. An algebraic route uses induction from finite
241
+ subgroups: the Farrell--Jones conjecture with complex coefficients
242
+ implies the complex Bass statement
243
+ \cite[Theorems 1.5 and 1.9]{BartelsLuckReich2008}.
244
+ The present proof uses the finite support of group-ring idempotents
245
+ throughout; it requires neither an assembly hypothesis nor a statement
246
+ about a completed group algebra.
247
+
248
+ For some groups, analytic methods give a stronger idempotent conclusion
249
+ in the reduced group $C^*$-algebra $C_r^*(G)$, the operator-norm closure
250
+ of $\C G$ acting on $\ell^2(G)$. Using Lafforgue's Banach $KK$-theory,
251
+ Mineyev and Yu proved this for torsion-free subgroups of hyperbolic groups
252
+ \cite[Theorems 19--21]{MineyevYu2002}. Puschnigg independently obtained
253
+ the torsion-free hyperbolic case through local cyclic homology
254
+ \cite{Puschnigg2002}; see also \cite[Section 6]{MineyevYu2002}.
255
+ Our conclusion for arbitrary torsion-free groups concerns the group ring
256
+ and the trace on its algebraic $K_0$, as distinguished in
257
+ Section~\ref{sec:torsion-free}.
258
+
259
+ The higher-dimensional algebraic construction has antecedents in the
260
+ cyclic-homological approach to the conjecture. Connes constructed a pairing
261
+ of even cyclic cocycles with projective classes
262
+ \cite[Part II, \S2, Proposition 14]{Connes1985}. Burghelea's decomposition
263
+ of cyclic homology by conjugacy classes identifies the infinite-order
264
+ components through the reduced centralizers $C_G(g)/\langle g\rangle$
265
+ \cite[Proposition 1.8 and Theorem I]{Burghelea1985}. Eckmann used
266
+ higher-degree vanishing to obtain trace vanishing over rational group
267
+ rings for specified classes of groups of finite rational homological
268
+ dimension \cite[\S3, Theorems 3.1 and 3.3]{Eckmann1986}.
269
+ Sections~\ref{sec:idempotents}--\ref{sec:detector} give direct finite-chain
270
+ constructions in this tradition, including the normalization of the
271
+ Pfaffian detector; no cyclic-homology theorem is needed as an input.
272
+ The sparse-chain theorem replaces a homological-dimension hypothesis
273
+ with connected-support control on the particular cycles.
274
+
275
+ The geometric proof develops the separating-set method of Papasoglu
276
+ \cite[\S2, especially Lemma 2.5]{Papasoglu2020}, the separating filtrations and simplex-counting
277
+ argument of Alpert \cite[Lemmas 4, 6--7]{Alpert2025}, and the
278
+ Cantor-parameter approach of Braun and Sauer
279
+ \cite[\S\S2, 4--5]{BraunSauer2021}. Alpert's equivariant formulations
280
+ \cite[\S4, especially Lemmas 11--12]{Alpert2025} provide the closest model
281
+ for the local comparisons. Alpert's filtration results concern manifold
282
+ geometry and compatible metrics. We give the full piecewise-linear argument needed
283
+ for simplex-dependent areas and arbitrary cycles in the coinvariant
284
+ chain complex. The separate Pfaffian calculation converts this
285
+ geometric vanishing into a statement about each conjugacy-class
286
+ coefficient.
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/02-framework.tex ADDED
@@ -0,0 +1,75 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A vanishing theorem for sparse simplicial cycles}
2
+ \label{sec:framework}
3
+
4
+ We formulate the geometric statement independently of group rings.
5
+ Its input is a graph with a free group action and a simplicial complex
6
+ whose top-dimensional vertex sets are connected in that graph. Its output
7
+ is the vanishing of every invariant cocycle evaluation in sufficiently
8
+ high dimension.
9
+
10
+ For a set $Y$, let $\C^{(Y)}$ be the vector space with basis
11
+ $\{\delta_y:y\in Y\}$, consisting of finite linear combinations. The
12
+ augmented chains of the full simplex on $Y$ are
13
+ \[
14
+ E_j=\bigwedge^{j+1}\C^{(Y)}\quad(j\geq0),\qquad E_{-1}=\C.
15
+ \]
16
+ The differential is contraction with the functional
17
+ $\alpha(\sum_y c_y\delta_y)=\sum_y c_y$:
18
+ \begin{equation}\label{eq:boundary}
19
+ \partial(\delta_{y_0}\wedge\cdots\wedge\delta_{y_j})
20
+ =\sum_{i=0}^{j}(-1)^i
21
+ \delta_{y_0}\wedge\cdots\wedge\widehat{\delta_{y_i}}
22
+ \wedge\cdots\wedge\delta_{y_j}.
23
+ \end{equation}
24
+ In degree zero this is the augmentation to $\C$; the empty wedge is $1$.
25
+ For a simplicial subcomplex $K$, its augmented oriented chains
26
+ $C_*(K)$ form a subcomplex of $E_*$.
27
+
28
+ If a group $H$ acts on $Y$, it acts on both chain complexes by permuting
29
+ vertices, with the signs prescribed by the exterior product. For an
30
+ $H$-module $V$, its coinvariants are
31
+ \[
32
+ V_H=V/\operatorname{span}_{\C}\{hv-v:h\in H,\ v\in V\}.
33
+ \]
34
+ The differentials induce differentials on coinvariants. A cycle in
35
+ $C_n(K)_H$ is a class whose boundary is zero there; an arbitrary finite
36
+ chain representing it need not have zero boundary before passage to
37
+ coinvariants. An $H$-invariant linear functional $\psi:E_n\to\C$
38
+ descends to $(E_n)_H$. We call it a cocycle when
39
+ $\psi\partial=0$ on $E_{n+1}$.
40
+
41
+ \begin{theorem}[Sparse-chain vanishing]\label{thm:sparse}
42
+ For each integer $D\geq2$ there is an integer $n_0(D)$ with the following
43
+ property. Let $Y$ be the vertex set of a countable connected simple graph
44
+ of degree at most $D$, and let a countable group $H$ act by graph
45
+ automorphisms, freely on vertices. Suppose $n\geq n_0(D)$ and $K$ is an
46
+ $H$-invariant subcomplex of the full simplex on $Y$ such that:
47
+ \begin{enumerate}[label=\textup{(\roman*)}]
48
+ \item $K$ is generated by its $n$-simplices and has finitely many
49
+ $H$-orbits of simplices;
50
+ \item the vertices of each $n$-simplex span a connected subgraph of $Y$.
51
+ \end{enumerate}
52
+ Then every $H$-invariant cocycle $\psi:E_n\to\C$ evaluates to zero on
53
+ the image in $(E_n)_H$ of every cycle in $C_n(K)_H$.
54
+ \end{theorem}
55
+
56
+ The bound $n_0(D)$ depends only on the graph degree, not on $H$, $K$ or
57
+ $\psi$. There is no boundedness hypothesis on $\psi$. We will bound it
58
+ only on a finite set of basis wedges associated with each fixed original
59
+ simplex. This distinction is necessary in the application.
60
+
61
+ For the proof assume $K\ne\varnothing$; the empty case has no positive
62
+ degree chains. Its realization $|K|$ consists of finitely supported
63
+ probability vectors $p:Y\to[0,1]$ whose supports are simplices of $K$.
64
+ A simplex will also denote its closed affine realization; $\sigma^\circ$
65
+ denotes its relative interior. We call simplices of $K$ \emph{original}
66
+ to distinguish them from the later subdivisions, and call its
67
+ $n$-simplices \emph{top simplices}.
68
+
69
+ The proof has three steps. First, we choose a metric and simplexwise
70
+ areas for which balls have small volume in high dimension.
71
+ Second, we construct separating filtrations with very few points in
72
+ their final stratum, on average over a free probability parameter.
73
+ Third, we use their subdivisions to construct equivariant chain maps
74
+ homotopic to inclusion whose cocycle evaluations approach zero. Each
75
+ approximation uses a finite filtration; no limiting filtration is needed.
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/03-metric.tex ADDED
@@ -0,0 +1,262 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A metric and volume bound for connected supports}
2
+ \label{sec:metric}
3
+
4
+ We work with the graph \(Y\), group \(H\), and nonempty
5
+ \(n\)-dimensional complex \(K\) of Theorem~\ref{thm:sparse}, where
6
+ \(n\geq1\). We need two kinds of geometric control: a metric with
7
+ finite neighborhoods in which to make cuts, and Euclidean area
8
+ functionals for which those cuts satisfy a slicing inequality.
9
+ We will use a scaled transportation metric on \(|K|\) and,
10
+ separately inside each top simplex, Euclidean structures determined
11
+ by its spanning trees. Each top simplex will have volume \(1/n!\),
12
+ while every affine branch of a distance function will have gradient
13
+ norm at most one in each of these structures. Counting the possible
14
+ connected vertex supports will then give the ball-volume estimate
15
+ used in the separating argument.
16
+
17
+ \subsection{The metric and its finite local geometry}
18
+
19
+ Represent a point of \(|K|\) by a probability vector \(p\) on \(Y\) whose
20
+ support lies in a simplex of \(K\). Let \(d_Y\) denote graph distance and
21
+ define
22
+ \begin{equation}
23
+ \rho(p,q)=\frac1{\sqrt n}
24
+ \sup_{\operatorname{Lip}_{d_Y}(\ell)\leq1}
25
+ \sum_{v\in Y}\ell(v)\bigl(p(v)-q(v)\bigr).
26
+ \label{eq:transport-metric}
27
+ \end{equation}
28
+ This is the scaled Kantorovich--Rubinstein metric on finitely
29
+ supported probability measures, in its Lipschitz-potential form
30
+ \cite[pp.~1381--1382]{Kantorovich2006}. We establish its needed
31
+ properties directly.
32
+ Only finitely many terms occur in the pairing. To see that the
33
+ supremum is finite and describe the distance function on each simplex,
34
+ let \(V\subset Y\) be a nonempty finite set and put
35
+ \[
36
+ \mathcal P_V=
37
+ \left\{\ell\in\R^V:
38
+ \sum_{v\in V}\ell(v)=0,\quad
39
+ |\ell(v)-\ell(w)|\leq d_Y(v,w)\quad(v,w\in V)\right\}.
40
+ \]
41
+ This is a nonempty compact polytope. Indeed, its difference constraints
42
+ and zero mean bound every coordinate by
43
+ \(\max_{v,w\in V}d_Y(v,w)\). Each \(\ell\in\mathcal P_V\) extends to
44
+ a \(1\)-Lipschitz function on \(Y\) by
45
+ \[
46
+ \widetilde\ell(y)=\min_{v\in V}\bigl(\ell(v)+d_Y(v,y)\bigr).
47
+ \]
48
+ The difference constraints show that this extension agrees with
49
+ \(\ell\) on \(V\), and the triangle inequality proves that it is
50
+ \(1\)-Lipschitz. Conversely, a global \(1\)-Lipschitz function restricts,
51
+ after subtraction of its mean, to an element of \(\mathcal P_V\).
52
+ Constants pair to zero with \(p-q\). Consequently, when \(V\) contains
53
+ both supports, the supremum in \eqref{eq:transport-metric} is the maximum
54
+ over \(\mathcal P_V\).
55
+
56
+ Symmetry follows by replacing \(\ell\) with \(-\ell\), and the triangle
57
+ inequality follows by applying each potential to
58
+ \(p-q=(p-u)+(u-q)\). The indicator of a single vertex is
59
+ \(1\)-Lipschitz for \(d_Y\), so
60
+ \begin{equation}
61
+ |p(v)-q(v)|\leq\sqrt n\,\rho(p,q)
62
+ \qquad(v\in Y).
63
+ \label{eq:coordinate-control}
64
+ \end{equation}
65
+ Thus \(\rho\) separates points and is a metric. It is \(H\)-invariant
66
+ because graph automorphisms permute the admissible potentials. On
67
+ probability vectors supported in a fixed finite set, it is the
68
+ restriction of a norm on the finite-dimensional space of vectors with
69
+ coordinate sum zero. It therefore gives the usual topology on every
70
+ finite subcomplex.
71
+
72
+ For \(c\in|K|\), write
73
+ \[
74
+ \begin{aligned}
75
+ f_c(p)&=\rho(c,p),& U_s(c)&=\{p:f_c(p)<s\},\\
76
+ L_s(c)&=\{p:f_c(p)\leq s\},& S_s(c)&=\{p:f_c(p)=s\}.
77
+ \end{aligned}
78
+ \]
79
+ On a fixed closed simplex \(\sigma\), the function \(f_c\) is a maximum
80
+ of finitely many affine functions: use the extreme points of
81
+ \(\mathcal P_{V(\sigma)\cup\supp c}\). Here \(V(\sigma)\) denotes the
82
+ vertex set of \(\sigma\). Taking all these extreme points makes the
83
+ collection of affine branches equivariant under \(H\).
84
+
85
+ \begin{lemma}\label{lem:proper}
86
+ Every closed \(\rho\)-ball meets only finitely many simplices of \(K\).
87
+ The complex \(K\) is locally finite, and \(\rho\) gives its usual
88
+ realization topology and is proper. For each \(c\in|K|\), \(s\geq0\),
89
+ and simplex \(\kappa\), the set
90
+ \[
91
+ \{h\in H:L_s(hc)\cap\kappa\ne\varnothing\}
92
+ \]
93
+ is finite. The setwise stabilizer \(H_\kappa\) of a nonempty simplex
94
+ is finite as well.
95
+ \end{lemma}
96
+
97
+ \begin{proof}
98
+ Let \(A=\supp c\). The function
99
+ \(d_Y(\,\cdot\,,A)\) is \(1\)-Lipschitz and vanishes on \(A\).
100
+ Using its negative in \eqref{eq:transport-metric} gives
101
+ \begin{equation}
102
+ \min_{\substack{a\in\supp c\\v\in\supp p}}d_Y(a,v)
103
+ \leq \sum_v p(v)d_Y(v,A)
104
+ \leq\sqrt n\,\rho(c,p).
105
+ \label{eq:support-distance}
106
+ \end{equation}
107
+ If a top simplex \(\sigma\) meets \(L_s(c)\) at \(p\), it therefore
108
+ contains a vertex within distance \(\lfloor s\sqrt n\rfloor\) of \(A\).
109
+ The graph on its \(n+1\) vertices is connected, so every vertex of
110
+ \(\sigma\) is within another \(n\) steps of that vertex. Thus all
111
+ such simplices use vertices in the finite graph neighborhood
112
+ \[
113
+ B^Y_{\lfloor s\sqrt n\rfloor+n}(A)
114
+ :=\{v\in Y:d_Y(v,A)\leq\lfloor s\sqrt n\rfloor+n\}.
115
+ \]
116
+ There are only finitely many possibilities for \(\sigma\) and its
117
+ faces. Likewise, every top simplex containing a specified vertex
118
+ \(v\) uses vertices in \(B^Y_n(\{v\})\); hence each vertex has a
119
+ finite star.
120
+
121
+ For completeness, the finite-subcomplex topology statement implies
122
+ the corresponding statement on all of \(|K|\). Given \(p\), let
123
+ \(\eta=\min\{p(v):v\in\supp p\}>0\). By
124
+ \eqref{eq:coordinate-control}, the ball of radius
125
+ \(\eta/(2\sqrt n)\) about \(p\) lies in the finite star of
126
+ \(\supp p\). Within this star the metric and realization topologies
127
+ agree. The open star of \(\supp p\) is also a neighborhood of \(p\)
128
+ in the locally finite realization, so the agreement is local in
129
+ both topologies. A closed metric ball is a closed subset of the
130
+ finite union of closed simplices it meets, and is therefore compact.
131
+
132
+ If \(L_s(hc)\) meets \(\kappa\), \eqref{eq:support-distance} supplies
133
+ \(a\in A\) and \(b\in V(\kappa)\) with
134
+ \(d_Y(ha,b)\leq s\sqrt n\). For each \(a\), the map \(h\mapsto ha\)
135
+ is injective because \(H\) acts freely on vertices. The finitely
136
+ many pairs \(a,b\) and finite graph balls therefore allow only
137
+ finitely many \(h\). Finally, for \(v\in V(\kappa)\), the same
138
+ injection maps \(H_\kappa\) into \(V(\kappa)\). In particular,
139
+ \(|H_\kappa|\leq|V(\kappa)|\).
140
+ \end{proof}
141
+
142
+ We will also use the following consequence. For fixed \(c\) and \(s\),
143
+ only finitely many \(h\in H\) satisfy
144
+ \begin{equation}
145
+ L_s(hc)\cap L_s(c)\ne\varnothing.
146
+ \label{eq:finite-ball-overlaps}
147
+ \end{equation}
148
+ Indeed, an intersection gives \(\rho(hc,c)\leq2s\), and then
149
+ \eqref{eq:support-distance} puts some vertex of \(h\supp c\)
150
+ within distance \(2s\sqrt n\) of \(\supp c\). The same
151
+ injectivity argument applies.
152
+
153
+ \subsection{Simplex areas and distance gradients}
154
+
155
+ The metric now provides finite neighborhoods in which we can make
156
+ cuts. For area comparisons, we use Euclidean structures separately
157
+ inside the top simplices. They need not agree on shared faces.
158
+
159
+ Fix a top simplex \(\sigma\). For each spanning tree \(T\) of the
160
+ connected graph on \(V(\sigma)\), equip its affine span with the
161
+ Euclidean structure in which the tree-edge vectors
162
+ \(\delta_v-\delta_w\), with either orientation for each edge, form
163
+ an orthonormal basis of the translation space. For \(0\leq j\leq n\),
164
+ let \(a_j^\sigma\) be the average, over these finitely many trees,
165
+ of Euclidean \(j\)-area on polyhedral subsets of \(\sigma^\circ\)
166
+ of dimension at most \(j\). We allow relatively open faces in
167
+ these sets; pieces of dimension less than \(j\) have zero
168
+ \(j\)-area, and \(a_0^\sigma\) is counting measure. These area
169
+ functionals are covariant under \(H\), since the action permutes
170
+ the spanning trees.
171
+
172
+ \begin{lemma}\label{lem:tree}
173
+ In every tree Euclidean structure on a top simplex \(\sigma\), its
174
+ \(n\)-volume is \(1/n!\). Every affine branch of \(f_c|_\sigma\)
175
+ has gradient of norm at most one, for every \(c\in|K|\).
176
+ The same gradient bound holds after restriction to any affine
177
+ subspace of the span of \(\sigma\).
178
+ \end{lemma}
179
+
180
+ \begin{proof}
181
+ Root the tree at \(v_0\), orient its edges away from the root, and
182
+ order the remaining vertices so that each parent precedes its
183
+ children. Put
184
+ \[
185
+ t_i=\delta_{v_i}-\delta_{\operatorname{parent}(v_i)},
186
+ \qquad b_i=\delta_{v_i}-\delta_{v_0}
187
+ \quad(1\leq i\leq n).
188
+ \]
189
+ Each \(b_i\) is the sum of the \(t_j\) along its root path.
190
+ Thus the change-of-basis matrix is triangular with diagonal
191
+ entries one. The \(t_i\) are an orthonormal basis in the chosen
192
+ metric, so the parallelepiped spanned by the \(b_i\) has volume
193
+ one. The simplex has volume \(1/n!\).
194
+
195
+ An affine branch has derivative along \(t_i\) equal, up to sign, to
196
+ \[
197
+ \frac{\ell(v_i)-\ell(\operatorname{parent}(v_i))}{\sqrt n}
198
+ \]
199
+ for a \(1\)-Lipschitz potential \(\ell\). Since the two vertices
200
+ are adjacent, this derivative has absolute value at most
201
+ \(1/\sqrt n\). The squared gradient norm is the sum of the
202
+ squares of these \(n\) derivatives and is at most one.
203
+ Restriction to an affine subspace replaces the gradient by its
204
+ orthogonal projection, which cannot increase its norm.
205
+ \end{proof}
206
+
207
+ \subsection{The volume margin in high dimension}
208
+
209
+ We next bound the total top-dimensional area of a metric ball by
210
+ counting its possible connected vertex supports. Fix
211
+ \[
212
+ R=4D^2,\qquad r=R/2.
213
+ \]
214
+ For a specified vertex \(v\), there are at most \(D^{2n}\)
215
+ connected sets of \(n+1\) vertices containing \(v\). To prove
216
+ this, choose a spanning tree of each such set rooted at \(v\).
217
+ A traversal using each tree edge once in each direction is a
218
+ walk of length \(2n\), starting at \(v\), whose visited set is
219
+ exactly the prescribed set. Choosing one such walk per set
220
+ gives an injection into the length-\(2n\) walks from \(v\),
221
+ of which there are at most \(D^{2n}\).
222
+
223
+ Set \(k=\lfloor R\sqrt n\rfloor\). A graph ball of radius \(k\)
224
+ has at most
225
+ \[
226
+ \sum_{j=0}^kD^j\leq D^{k+1}
227
+ \]
228
+ vertices, since \(D\geq2\). As \(|\supp c|\leq n+1\), there are
229
+ at most \((n+1)D^{k+1}\) vertices within distance \(k\) of
230
+ \(\supp c\). By \eqref{eq:support-distance}, each top simplex
231
+ meeting \(L_R(c)\) contains one of them. The connected-set
232
+ count and Lemma~\ref{lem:tree} therefore give, for every \(c\in|K|\),
233
+ \begin{equation}
234
+ \sum_{\sigma\ \mathrm{top}}
235
+ a_n^\sigma\bigl(L_R(c)\cap\sigma^\circ\bigr)
236
+ \leq V_R:=
237
+ \frac{(n+1)D^{\lfloor R\sqrt n\rfloor+1}D^{2n}}{n!}.
238
+ \label{eq:volume-bound}
239
+ \end{equation}
240
+ Counting a simplex more than once only enlarges this upper bound.
241
+
242
+ With \(D\) fixed, the ratio of this estimate to
243
+ \((R-r)^n/n!\) is
244
+ \[
245
+ \frac{V_R}{(R-r)^n/n!}
246
+ =\frac{(n+1)D^{\lfloor4D^2\sqrt n\rfloor+1}}{2^n}
247
+ \longrightarrow0.
248
+ \]
249
+ Indeed, its logarithm is
250
+ \(-n\log2+4D^2(\log D)\sqrt n+O_D(\log n)\).
251
+ We may therefore choose \(n_0(D)\geq1\) so that, for every
252
+ \(n\geq n_0(D)\),
253
+ \begin{equation}
254
+ V_R<\frac{(R-r)^n}{n!}.
255
+ \label{eq:strict-volume}
256
+ \end{equation}
257
+ For the remainder of the geometric proof, fix such an \(n\).
258
+ The graph degree bound \(D\), and hence \(R\) and \(r\), remain
259
+ fixed as dimensions increase. The strict margin
260
+ \eqref{eq:strict-volume} will convert successive area comparisons
261
+ into a bound on the number of points at the bottom of a
262
+ separating filtration.
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/04-filtrations.tex ADDED
@@ -0,0 +1,276 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Equivariant separating filtrations}\label{sec:filtrations}
2
+
3
+ We retain the complex $K$, the metric $\rho$, and the radii $r<R$
4
+ from Section~\ref{sec:metric}. We will repeatedly cut $K$ into pieces of
5
+ diameter at most $2R$, lowering the dimension of the separating set at
6
+ each step. The cuts vary over a compact probability space on which $H$
7
+ acts freely. This allows local modifications to be separated after
8
+ taking account of the parameter, even when their translates overlap in
9
+ $|K|$.
10
+
11
+ \subsection{A free probability parameter}
12
+
13
+ The following construction is a finite-color variant of the coinduction
14
+ argument in Braun and Sauer \cite[Theorem 2.1]{BraunSauer2021}, who credit
15
+ the existence theorem to Hjorth and Molberg \cite[Theorem 0.1]{HjorthMolberg2006}.
16
+ We include the construction,
17
+ including its torsion case, so that no free-action theorem is an input.
18
+
19
+ \begin{lemma}\label{lem:free-parameter}
20
+ Every countable group $H$ admits a continuous free action on a compact
21
+ metrizable zero-dimensional space $X$, preserving a Borel probability
22
+ measure $\mu$.
23
+ \end{lemma}
24
+
25
+ \begin{proof}
26
+ For $a\in H\setminus\{1\}$, put $k_a=\operatorname{ord}(a)$ if $a$ has
27
+ finite order, and $k_a=2$ otherwise. Let
28
+ \[
29
+ X_a=\{\xi:H\longrightarrow\Z/k_a\Z:
30
+ \xi(ta)=\xi(t)+1\text{ for every }t\in H\}.
31
+ \]
32
+ This is a closed subspace of the product of finite discrete spaces
33
+ $(\Z/k_a\Z)^H$. Choose a representative $t_C$ for each left coset
34
+ $C=t_C\langle a\rangle$. A coloring in $X_a$ is specified uniquely by
35
+ offsets $\omega_C\in\Z/k_a\Z$, through
36
+ $\xi(t_Ca^j)=\omega_C+j$. This is well defined also when $a$ has finite
37
+ order, because the modulus is then its order. Thus $X_a$ is nonempty,
38
+ compact and zero-dimensional.
39
+
40
+ Give the offsets independent uniform distributions. The left action
41
+ \[
42
+ (h\xi)(t)=\xi(h^{-1}t)
43
+ \]
44
+ preserves $X_a$ and its probability measure: it permutes the cosets and
45
+ adds a fixed element of $\Z/k_a\Z$ to each offset. These operations
46
+ preserve every finite cylinder probability. Take the product over
47
+ $a\ne1$ to obtain $X$ and $\mu$. Countability gives metrizability, and
48
+ the coordinatewise action is continuous and measure preserving.
49
+ For any $a\ne1$ and any point of $X$, its $a$-coordinate satisfies
50
+ \[
51
+ (a\xi_a)(1)=\xi_a(a^{-1})=\xi_a(1)-1\ne\xi_a(1).
52
+ \]
53
+ Hence no nonidentity element fixes a point. If $H$ is trivial, take a
54
+ one-point probability space.
55
+ \end{proof}
56
+
57
+ Fix such $(X,\mu)$ for the rest of the geometric argument. In
58
+ particular, no amenability assumption on $H$ is needed.
59
+
60
+ \subsection{The allowed filtrations}
61
+
62
+ A triangulation refining $K$ means a finite affine simplicial
63
+ subdivision of each closed original simplex, with agreement on shared
64
+ faces. A family $T(x)$ of such triangulations, together with specified
65
+ subcomplexes, is \emph{locally constant} if, on each original simplex,
66
+ all its exact affine simplices and subcomplex markings are constant on
67
+ the pieces of a finite clopen partition of $X$. The partition may
68
+ depend on the original simplex. We require equivariance:
69
+ $T(hx)=hT(x)$, and likewise for every specified subcomplex.
70
+ Refinement of triangulations always preserves their earlier
71
+ subcomplexes.
72
+
73
+ Begin with $T_n(x)=K$ and $Z_n(x)=|K|$. At stage $d$, where
74
+ $n\ge d\ge1$, suppose that $P(x)=Z_d(x)$ is a subcomplex of $T_d(x)$.
75
+ An \emph{admissible} next choice consists of a locally constant equivariant
76
+ refinement $T_{d-1}(x)$ and its subcomplex $Z_{d-1}(x)$ such that
77
+ \begin{enumerate}[label=\textup{(\roman*)}]
78
+ \item $Z_{d-1}(x)\subseteq P(x)$;
79
+ \item for every simplex $F$ of $T_d(x)$ contained in $P(x)$,
80
+ \[
81
+ \dim\bigl(F\cap Z_{d-1}(x)\bigr)\le\dim F-1;
82
+ \]
83
+ \item every connected component of $P(x)\setminus Z_{d-1}(x)$ has
84
+ $\rho$-diameter at most $2R$.
85
+ \end{enumerate}
86
+ A negative dimension bound means that the intersection is empty.
87
+ Thus the new separator avoids the vertices of $T_d$ and meets each
88
+ higher-dimensional face in lower dimension; its own vertices belong to
89
+ the finer triangulation $T_{d-1}$.
90
+ Connected components use the subspace topology given by $\rho$.
91
+ We call a filtration satisfying these conditions admissible.
92
+ In particular, these conditions imply $\dim Z_i(x)\le i$.
93
+
94
+ The local operation behind the construction is easiest to describe at a
95
+ fixed parameter. For a separator $Z\subseteq P$, a center $c\in|K|$,
96
+ and $t\in(r,R)$, remove the part of $Z$ inside the ball and insert
97
+ the corresponding slice of $P$:
98
+ \[
99
+ Z^{\prime}=(Z\setminus U_t(c))\cup(P\cap S_t(c)).
100
+ \]
101
+ The inserted slice prevents a component of $P\setminus Z^{\prime}$
102
+ from passing between the ball and its exterior. Inside the ball its
103
+ diameter is at most $2t$; outside, the old separator remains.
104
+ The next lemma makes this operation compatible with triangulations,
105
+ group translates, and clopen parameter choices. It also constructs the
106
+ level cuts used to start a filtration. Only the affine descriptions of
107
+ distance levels enter the construction; no Euclidean metrics need to
108
+ agree across faces.
109
+
110
+ \begin{lemma}[Compatible cuts]\label{lem:refinement}
111
+ Fix locally constant equivariant triangulation families $T$ and $S$,
112
+ where $S$ refines $T$, and subcomplex families $P\subseteq T$ and
113
+ $Z\subseteq S$ with $Z\subseteq P$. Let
114
+ $\{(c_\alpha,B_\alpha)\}_{\alpha\in A}$ be a countable equivariant
115
+ family of centers $c_\alpha\in|K|$ and clopen sets $B_\alpha\subseteq X$.
116
+ Assume that only finitely many of the balls $L_R(c_\alpha)$ meet any
117
+ given original simplex. Set
118
+ \[
119
+ \mathcal U_t(x)=\bigcup_{\alpha:\,x\in B_\alpha}U_t(c_\alpha),
120
+ \qquad
121
+ \mathcal S_t(x)=\bigcup_{\alpha:\,x\in B_\alpha}S_t(c_\alpha).
122
+ \]
123
+ Outside a countable set of radii $t\in(r,R)$, there is a locally
124
+ constant equivariant triangulation refining $S$ in which both
125
+ \begin{equation}\label{eq:cut-replacement}
126
+ \begin{gathered}
127
+ P(x)\cap\mathcal S_t(x),\\
128
+ \bigl(Z(x)\setminus\mathcal U_t(x)\bigr)
129
+ \cup\bigl(P(x)\cap\mathcal S_t(x)\bigr)
130
+ \end{gathered}
131
+ \end{equation}
132
+ are subcomplexes. Each inserted level meets every face $F$ of $T$ or
133
+ $S$ in dimension at most $\dim F-1$. Consequently, if $Z$ satisfies
134
+ the dimension-drop condition relative to $T$, both displayed sets do
135
+ also. If every component of $P\setminus Z$ has diameter at most $2R$,
136
+ the second displayed set preserves that property.
137
+ \end{lemma}
138
+
139
+ \begin{proof}
140
+ On a fixed original simplex the function
141
+ $f_c(p)=\rho(c,p)$ is a maximum of finitely many affine functions.
142
+ For a fixed face $F$, a level $\{f_c=t\}$ can have full dimension in
143
+ $F$ only if one of these affine functions is identically $t$ on the
144
+ affine span of $F$. Otherwise the level is contained in a finite
145
+ union of proper affine hyperplanes. Thus only finitely many levels
146
+ are exceptional for this face and center. There are countably many
147
+ original simplices and centers, and only finitely many exact
148
+ triangulation types on each original simplex. Excluding the
149
+ resulting countable union of exceptional levels gives the stated
150
+ dimension drop simultaneously for all faces of $T$ and $S$.
151
+
152
+ We give the compatible refinement explicitly. On each original
153
+ simplex $\sigma$, cut the simplices of $S$ by all hyperplanes $b=t$,
154
+ where $b$ is an affine branch for one of the finitely many relevant
155
+ centers. Use the
156
+ canonical branch collection from the finite potential polytope in
157
+ Section~\ref{sec:metric}. On each piece of the finite clopen partition
158
+ recording the old data and active conditions, this gives a finite
159
+ polytopal complex $\mathcal P_\sigma$. It represents the old
160
+ subcomplexes and the closed conditions defining the two sets in
161
+ \eqref{eq:cut-replacement}.
162
+
163
+ These polytopal complexes may initially disagree on original faces.
164
+ For each original simplex $\tau$, let $\mathcal Q_\tau$ be the common
165
+ polytopal refinement of
166
+ \[
167
+ \mathcal P_\sigma|_\tau
168
+ \quad\text{over all original cofaces }\sigma\supseteq\tau,
169
+ \quad\text{including }\sigma=\tau.
170
+ \]
171
+ There are finitely many cofaces by Lemma~\ref{lem:proper}.
172
+ The common refinement consists of the nonempty intersections of cells
173
+ and their faces. If $\tau$ is a face of $\sigma$, then
174
+ $\mathcal Q_\tau$ refines $\mathcal Q_\sigma|_\tau$, since every coface
175
+ of $\sigma$ is also a coface of $\tau$.
176
+
177
+ Triangulate the original simplices in increasing dimension. When
178
+ handling $\sigma$, its boundary has already been triangulated by a
179
+ refinement of the boundary restrictions of $\mathcal Q_\sigma$.
180
+ Extend this triangulation over the cells of $\mathcal Q_\sigma$ in
181
+ increasing cell dimension. Keep cells in the original boundary as
182
+ already triangulated. For every other positive-dimensional cell,
183
+ cone its triangulated boundary to the arithmetic mean of its vertices,
184
+ which lies in its relative interior. Zero-dimensional cells need no
185
+ operation. The cones agree on common faces and give the desired finite
186
+ affine subdivision, preserving the prescribed boundary triangulation.
187
+
188
+ Every operation commutes with the affine maps induced by $H$:
189
+ restriction, common refinement, and the mean of the full vertex set of
190
+ a polytope are all canonical. This proves equivariance even for
191
+ nontrivial simplex stabilizers. On each original simplex the procedure
192
+ uses only finitely many data: those on its faces and their original
193
+ cofaces, together with finitely many relevant cuts. A common finite
194
+ clopen partition makes all these data constant. Thus the output has
195
+ the required local constancy. No manifold condition on $K$ is involved.
196
+
197
+ The first set in \eqref{eq:cut-replacement} has the dimension bound
198
+ already proved for the levels. The second is contained in the union
199
+ of those levels with $Z$, so it has the same bound whenever $Z$ does.
200
+ For its separation property, let $C$ be a component of its complement
201
+ in $P(x)$. If $C$ meets an active $U_t(c_\alpha)$, continuity of
202
+ $f_{c_\alpha}$ and connectedness of $C$ imply that $C$ stays in that
203
+ ball, since it avoids the inserted level. Its diameter is then at
204
+ most $2t<2R$. Otherwise $C$ lies outside all active open balls, where
205
+ the old set $Z$ was retained. It is therefore contained in an old
206
+ component of $P(x)\setminus Z(x)$ and has diameter at most $2R$.
207
+ \end{proof}
208
+
209
+ The genericity against $S$ is useful when $S$ already contains the old
210
+ separator $Z$: intersections of an inserted level with its faces have
211
+ one less dimension. The later area comparison will use precisely
212
+ this conclusion. The lemma itself does not require disjoint active
213
+ balls; disjointness will be imposed when their areas are counted.
214
+
215
+ \begin{lemma}\label{lem:filtration-exists}
216
+ For any allowed choices through stage $d$, an allowed choice of
217
+ $(T_{d-1},Z_{d-1})$ exists. Hence a filtration can be continued to
218
+ $Z_0$.
219
+ \end{lemma}
220
+
221
+ \begin{proof}
222
+ Each original simplex is compact in $\rho$. Cover representatives of
223
+ the finitely many original simplex orbits by finitely many open balls
224
+ $U_r(c)$, and take all their $H$-translates. These balls cover $|K|$.
225
+ By Lemma~\ref{lem:proper}, only finitely many translated radius-$R$
226
+ balls meet a given original simplex. Apply Lemma~\ref{lem:refinement}
227
+ with every activation set equal to $X$, with $T=S=T_d$, and with
228
+ $Z=\varnothing$. For a common allowed radius $t\in(r,R)$, take
229
+ \[
230
+ Z_{d-1}(x)=Z_d(x)\cap\bigcup_c S_t(c).
231
+ \]
232
+ This is a subcomplex of the resulting refinement and has the required
233
+ dimension drop. If $C$ is a component of $Z_d(x)\setminus Z_{d-1}(x)$,
234
+ choose $p\in C$ and a covering ball $U_r(c)$ containing it.
235
+ The connected set $f_c(C)$ avoids $t$ and contains a value below $t$,
236
+ so $C\subseteq U_t(c)$. Its diameter is at most $2t<2R$.
237
+ The assertion is vacuous for an empty component space.
238
+ \end{proof}
239
+
240
+ \subsection{Dimension drop along the entire filtration}
241
+
242
+ We record the consequence that will control chains in
243
+ Section~\ref{sec:chains}. For any simplex $F$ of $T_i(x)$ contained in
244
+ $Z_i(x)$ and any $0\le j\le i$,
245
+ \begin{equation}\label{eq:iterated-drop}
246
+ \dim\bigl(F\cap Z_j(x)\bigr)\le\dim F-(i-j).
247
+ \end{equation}
248
+ Indeed, the first step is the defining condition. Its intersection is
249
+ a subcomplex in the next refinement. Applying the next dimension
250
+ drop to each simplex of that subcomplex decreases its maximal
251
+ dimension by one. Induction gives \eqref{eq:iterated-drop}.
252
+ Applied with $i=n$, this also shows that a proper original face meets
253
+ $Z_j(x)$ in dimension strictly less than $j$.
254
+
255
+ \begin{lemma}[Carriers of the zero-dimensional stratum]\label{lem:carrier}
256
+ Let $(T_i,Z_i)_{i=0}^n$ be an allowed filtration and let $z\in Z_0(x)$.
257
+ For every $i$, there is a unique $i$-simplex of $T_i(x)$ contained in
258
+ $Z_i(x)$ and containing $z$. The point $z$ lies in its relative
259
+ interior. In particular, every point of $Z_0(x)$ lies in the interior
260
+ of an original top simplex.
261
+ \end{lemma}
262
+
263
+ \begin{proof}
264
+ Let $F$ be the unique simplex of $T_i(x)$ whose relative interior
265
+ contains $z$. Since $Z_i(x)$ is a subcomplex containing $z$, it contains
266
+ $F$, and $\dim F\le i$. If $\dim F<i$, then
267
+ \eqref{eq:iterated-drop} with $j=0$ would make $F\cap Z_0(x)$ empty.
268
+ Thus $\dim F=i$. Every other simplex containing $z$ has $F$ as a face,
269
+ so no other $i$-simplex contains it. Taking $i=n$ proves the last
270
+ assertion.
271
+ \end{proof}
272
+
273
+ We have obtained a nonempty class of equivariant separating
274
+ filtrations, together with a local cutting operation that stays within
275
+ that class. The next section chooses separators with area close to
276
+ the infimum and compares them with these cuts.
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/05-surgery.tex ADDED
@@ -0,0 +1,249 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Local replacement and the number of zero strata}
2
+ \label{sec:surgery}
3
+
4
+ We now choose the separating filtration so that its zero-dimensional set
5
+ has small expected cardinality in each original simplex. Throughout this
6
+ section the graph, complex, parameter space, dimension, and radii are fixed
7
+ as in Sections~\ref{sec:metric} and~\ref{sec:filtrations}. In particular,
8
+ the strict inequality~\eqref{eq:strict-volume} holds. Only the filtration
9
+ will depend on a positive number $\epsilon$.
10
+
11
+ \begin{proposition}\label{prop:zero-strata}
12
+ For every $\epsilon>0$ there is an admissible equivariant locally constant
13
+ filtration $(Z_j,T_j)_{j=0}^n$ such that, for every original top simplex
14
+ $\sigma$ of $K$,
15
+ \begin{equation}\label{eq:zero-strata}
16
+ \int_X\#\bigl(Z_0(x)\cap\sigma\bigr)\,d\mu(x)
17
+ \le C_\sigma\epsilon.
18
+ \end{equation}
19
+ Here $C_\sigma$ depends on the fixed geometric data but is independent of
20
+ $\epsilon$ and of the complexity of the chosen triangulations.
21
+ \end{proposition}
22
+
23
+ \subsection{Successive near minimizers}
24
+
25
+ The comparison with a cut through a ball follows the separating-set
26
+ method of Papasoglu \cite[Section 2, especially Lemma 2.5]{Papasoglu2020}
27
+ and its iterated and equivariant forms in Alpert
28
+ \cite[Lemmas 6--7 and 11--12]{Alpert2025}. We prove the comparisons for our
29
+ simplex-dependent areas, retaining the error from each near minimizer.
30
+
31
+ \begin{proof}[Proof of Proposition~\ref{prop:zero-strata}]
32
+ For an equivariant family $Z$ of dimension at most $j$, define
33
+ \begin{equation}\label{eq:normalized-area}
34
+ \mathcal I_j(Z)=
35
+ \sum_{\sigma\ \mathrm{top}\bmod H}\frac{1}{|H_\sigma|}
36
+ \int_X a_j^\sigma\bigl(Z(x)\cap\sigma^\circ\bigr)\,d\mu(x).
37
+ \end{equation}
38
+ The sum runs over representatives of the original top simplices, and
39
+ $H_\sigma$ is the finite setwise stabilizer of $\sigma$. This quantity is
40
+ finite for an admissible family. There are finitely many representatives,
41
+ and, on each, local constancy and compactness of $X$ give finitely many
42
+ finite polyhedral configurations, each of finite area.
43
+
44
+ Start with $(Z_n,T_n)=(|K|,K)$. At step $d=n,\ldots,1$, keep all previously
45
+ chosen data fixed and choose the admissible pair $(Z_{d-1},T_{d-1})$ so that
46
+ $\mathcal I_{d-1}(Z_{d-1})$ is within $\epsilon$ of the infimum over the
47
+ admissible choices at this step. Lemma~\ref{lem:filtration-exists} ensures
48
+ that this class is nonempty. Its infimum is a finite nonnegative number,
49
+ so such a choice exists. Consequently, for every admissible replacement
50
+ $Z'$ at this step,
51
+ \begin{equation}\label{eq:near-minimality}
52
+ \mathcal I_{d-1}(Z_{d-1})
53
+ \le \mathcal I_{d-1}(Z')+\epsilon.
54
+ \end{equation}
55
+ Neither an attained minimum nor a limit of filtrations is used.
56
+
57
+ \subsection{Disjoint replacements in the parameter and spatial variables}
58
+
59
+ Fix a center $c\in|K|$. The set
60
+ \[
61
+ \mathcal F_c=
62
+ \{h\in H\setminus\{1\}:L_R(hc)\cap L_R(c)\ne\varnothing\}
63
+ \]
64
+ is finite. Indeed such an intersection implies $\rho(hc,c)\le2R$;
65
+ the support-distance bound, the finite graph balls and freeness on vertices
66
+ then leave only finitely many possibilities for $h$.
67
+
68
+ There is a finite clopen partition of $X$ into sets $A$ satisfying
69
+ $A\cap hA=\varnothing$ for every $h\in\mathcal F_c$. To construct one,
70
+ use the free action and the zero-dimensional Hausdorff topology to choose,
71
+ around each $x\in X$, a clopen neighborhood disjoint from its translates
72
+ by this finite set. A finite subcover exists by compactness; the atoms of
73
+ its common refinement have the required property. Thus
74
+ \begin{equation}\label{eq:product-disjointness}
75
+ \{hA\times L_R(hc):h\in H\}
76
+ \quad\text{is a pairwise disjoint family.}
77
+ \end{equation}
78
+ This partition is fixed independently of $\epsilon$. The assertion
79
+ concerns the product of parameter and spatial variables; the sets $hA$
80
+ alone need not be disjoint.
81
+
82
+ Fix one atom $A$ and any clopen subset $B\subseteq A$. For $r\le s\le R$
83
+ put
84
+ \begin{equation}\label{eq:local-areas}
85
+ M_j(s)=\int_B\sum_{\sigma\ \mathrm{top}}
86
+ a_j^\sigma\bigl(Z_j(x)\cap\sigma^\circ\cap L_s(c)\bigr)\,d\mu(x),
87
+ \qquad 0\le j\le n.
88
+ \end{equation}
89
+ For a generic $t\in(r,R)$, also put
90
+ \[
91
+ N_{d-1}(t)=\int_B\sum_{\sigma\ \mathrm{top}}
92
+ a_{d-1}^\sigma
93
+ \bigl(Z_d(x)\cap\sigma^\circ\cap S_t(c)\bigr)\,d\mu(x).
94
+ \]
95
+ These sums involve only finitely many original simplices. Unlike
96
+ \eqref{eq:normalized-area}, they run over all such simplices and carry no
97
+ stabilizer weights.
98
+
99
+ At stage $d$, write $P=Z_d$ and $Z=Z_{d-1}$. For each $x$, make the
100
+ simultaneous replacement
101
+ \begin{equation}\label{eq:local-replacement}
102
+ Z'(x)=
103
+ \left(Z(x)\setminus\bigcup_{h:x\in hB}U_t(hc)\right)
104
+ \cup
105
+ \left(P(x)\cap\bigcup_{h:x\in hB}S_t(hc)\right).
106
+ \end{equation}
107
+ The active closed balls are pairwise disjoint by
108
+ \eqref{eq:product-disjointness}. The families of balls and levels are
109
+ locally finite, and their use is conditioned on clopen sets, so the
110
+ construction is equivariant and locally constant on every original
111
+ simplex. Apply Lemma~\ref{lem:refinement} with $T=T_d$,
112
+ $S=T_{d-1}$, $P=Z_d$, $Z=Z_{d-1}$, and the centers and activation
113
+ sets $(hc,hB)$. Outside a countable set of levels, it represents
114
+ $Z'$ by an admissible common refinement: the inserted levels have
115
+ the required dimension drop on faces of $T_d$ and of the old finer
116
+ triangulation $T_{d-1}$, and the lemma preserves the diameter bound
117
+ on components of $P(x)\setminus Z'(x)$.
118
+
119
+ We next compute the change in~\eqref{eq:normalized-area}. Genericity
120
+ against the faces of $T_{d-1}$ implies that the old set $Z$ meets any
121
+ inserted level in dimension at most $d-2$. When $d=1$, that intersection
122
+ is empty. Hence the removed $(d-1)$-area is unchanged if the open ball is
123
+ replaced by its closure, and the inserted cut has zero $(d-1)$-area
124
+ overlap with the retained old set.
125
+
126
+ The normalization in~\eqref{eq:normalized-area} makes the removed area
127
+ exactly $M_{d-1}(t)$ and the inserted area exactly $N_{d-1}(t)$. Here is
128
+ the orbit-counting identity behind this assertion. Let $Q$ denote the
129
+ relevant equivariant set, and let $W(c)$ denote either the ball or the
130
+ level. Covariance of area and invariance of $\mu$ give
131
+ \begin{align*}
132
+ &\sum_{\sigma\ \mathrm{top}\bmod H}\frac1{|H_\sigma|}
133
+ \sum_{h\in H}\int_{hB}
134
+ a_j^\sigma\bigl(Q(x)\cap\sigma^\circ\cap W(hc)\bigr)\,d\mu(x)
135
+ \\
136
+ &\quad=\sum_{\sigma\ \mathrm{top}\bmod H}\frac1{|H_\sigma|}
137
+ \sum_{h\in H}\int_B
138
+ a_j^{h^{-1}\sigma}
139
+ \bigl(Q(x)\cap(h^{-1}\sigma)^\circ\cap W(c)\bigr)\,d\mu(x)
140
+ \\
141
+ &\quad=\int_B\sum_{\tau\ \mathrm{top}}
142
+ a_j^\tau\bigl(Q(x)\cap\tau^\circ\cap W(c)\bigr)\,d\mu(x).
143
+ \end{align*}
144
+ The map $h\mapsto h^{-1}\sigma$ takes each value in the simplex orbit
145
+ exactly $|H_\sigma|$ times. All local contributions are nonnegative,
146
+ and only finitely many translates meet any fixed representative simplex.
147
+ The disjointness and zero-overlap statements above therefore yield
148
+ \[
149
+ \mathcal I_{d-1}(Z')-\mathcal I_{d-1}(Z)
150
+ =N_{d-1}(t)-M_{d-1}(t).
151
+ \]
152
+ Combining this identity with~\eqref{eq:near-minimality} gives
153
+ \begin{equation}\label{eq:local-comparison}
154
+ M_{d-1}(t)\le N_{d-1}(t)+\epsilon
155
+ \quad\text{for almost every }t\in(r,R).
156
+ \end{equation}
157
+
158
+ \subsection{Slicing and the strict volume margin}
159
+
160
+ We have compared the area of a separating set inside a ball with that
161
+ of a cut through the preceding set. Slicing now connects these
162
+ comparisons across the successive dimensions.
163
+
164
+ Work first in one original top simplex $\sigma$ and one of its tree
165
+ metrics. Decompose $Z_d(x)\cap\sigma^\circ$ into affine polyhedral
166
+ pieces on which $f_c=\rho(c,\cdot)$ is affine. On a $d$-dimensional
167
+ piece $Q$, its tangential gradient has norm $\alpha\le1$ by
168
+ Lemma~\ref{lem:tree}. Euclidean slicing perpendicular to that gradient
169
+ gives
170
+ \[
171
+ \int_r^b\operatorname{vol}_{d-1}(Q\cap\{f_c=t\})\,dt
172
+ =\alpha\operatorname{vol}_d(Q\cap\{r<f_c<b\})
173
+ \le\operatorname{vol}_d(Q\cap L_b(c)).
174
+ \]
175
+ A constant branch contributes at only one level. Pieces of dimension
176
+ less than $d$, including interfaces of this decomposition, have zero
177
+ $(d-1)$-slice area outside finitely many exceptional levels. Averaging
178
+ over the tree metrics, summing over original top interiors, and
179
+ integrating over $B$ yields
180
+ \begin{equation}\label{eq:coarea}
181
+ \int_r^bN_{d-1}(t)\,dt\le M_d(b),\qquad r\le b\le R.
182
+ \end{equation}
183
+ These operations are legitimate by local finiteness and local constancy;
184
+ on the fixed ball only finitely many configurations are involved.
185
+ Every comparison has taken place in a single simplex metric before
186
+ averaging, so no compatibility of metrics across original faces is needed.
187
+ Indeed~\eqref{eq:iterated-drop} bounds $Z_d$ on a proper original face
188
+ by dimension $d-1$, and its generic level slice by dimension $d-2$.
189
+ Such faces contribute no area to the preceding comparison. The same
190
+ dimension estimate says that $Z_0$ misses every proper original face.
191
+
192
+ From~\eqref{eq:local-comparison} and~\eqref{eq:coarea},
193
+ \[
194
+ M_d(b)\ge\int_r^bM_{d-1}(t)\,dt-\epsilon(b-r).
195
+ \]
196
+ Induction, beginning with the monotonicity of $M_0$, gives
197
+ \[
198
+ M_d(b)\ge
199
+ \frac{(b-r)^d}{d!}M_0(r)
200
+ -\epsilon\sum_{i=1}^d\frac{(b-r)^i}{i!}.
201
+ \]
202
+ Set
203
+ \[
204
+ L=R-r,\qquad A_n=\frac{L^n}{n!},\qquad
205
+ \mathcal E_n=\sum_{i=1}^n\frac{L^i}{i!}.
206
+ \]
207
+ Since $Z_n=|K|$, the volume bound~\eqref{eq:volume-bound} implies
208
+ \begin{equation}\label{eq:iterated-volume}
209
+ A_nM_0(r)\le V_R\mu(B)+\epsilon \mathcal E_n.
210
+ \end{equation}
211
+
212
+ We may now choose
213
+ \[
214
+ B=A\cap\{x\in X:Z_0(x)\cap L_r(c)\ne\varnothing\}.
215
+ \]
216
+ This set is clopen: finitely many original simplices meet the ball, and
217
+ their exact filtration data are constant on a common finite clopen
218
+ partition. Although $B$ uses the completed filtration, its use in an
219
+ earlier comparison is legitimate. Inequality~\eqref{eq:near-minimality}
220
+ holds for every admissible competitor with the data down to stage $d$
221
+ fixed; it imposes no condition on the later stages. The same $B$ can
222
+ therefore be used in every comparison leading to
223
+ \eqref{eq:iterated-volume}.
224
+
225
+ Each $x\in B$ contributes at least one zero stratum, and each such point
226
+ lies in a unique original top interior. Thus $\mu(B)\le M_0(r)$.
227
+ Moreover $M_0(r)$ is the integral of the point count over all of $A$,
228
+ because that count is zero on $A\setminus B$. The strict inequality
229
+ $V_R<A_n$ now gives the direct expected-count bound
230
+ \begin{equation}\label{eq:ball-zero-strata}
231
+ \int_A\#\bigl(Z_0(x)\cap L_r(c)\bigr)\,d\mu(x)
232
+ =M_0(r)\le\frac{\mathcal E_n}{A_n-V_R}\,\epsilon.
233
+ \end{equation}
234
+
235
+ To pass from the ball estimate to \eqref{eq:zero-strata}, cover a fixed
236
+ original top simplex $\sigma$ by finitely many open
237
+ $r$-balls with fixed centers $c_1,\ldots,c_q$. Such a cover exists by
238
+ compactness of the simplex. For each center, use the fixed clopen
239
+ partition constructed above, and write $p_i$ for its number of atoms.
240
+ Sum~\eqref{eq:ball-zero-strata} over these atoms and then over the balls.
241
+ Since the corresponding closed balls also cover $\sigma$, this proves
242
+ \eqref{eq:zero-strata} with
243
+ \[
244
+ C_\sigma=\frac{\mathcal E_n}{A_n-V_R}\sum_{i=1}^q p_i.
245
+ \]
246
+ All quantities in this constant were fixed independently of $\epsilon$.
247
+ In particular, no bound on the number of subdivision simplices or on
248
+ the cardinality of an individual zero-dimensional fiber is needed.
249
+ \end{proof}
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/06-chains.tex ADDED
@@ -0,0 +1,324 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{From separating filtrations to finite chains}\label{sec:chains}
2
+
3
+ Fix the dimension $n$ and radii chosen in Section~\ref{sec:metric}.
4
+ For each $\epsilon>0$, use the filtration supplied by
5
+ Proposition~\ref{prop:zero-strata}. We will turn it into an
6
+ $H$-equivariant chain map
7
+ \[
8
+ F^\epsilon:C_*(K)\longrightarrow E_*
9
+ \]
10
+ that is equivariantly chain homotopic to inclusion. Its evaluation by
11
+ a fixed invariant cocycle will tend to zero. These two properties
12
+ prove Theorem~\ref{thm:sparse}. Throughout this section $n$ remains
13
+ fixed while $\epsilon$ tends to zero.
14
+
15
+ \subsection{Component averages and their finite support}
16
+
17
+ For a fixed parameter $x$, take the barycentric subdivision of the
18
+ final triangulation $T_0(x)$. Its vertices are the barycenters $b_F$
19
+ of nonempty simplices $F$ of $T_0(x)$. Define
20
+ \[
21
+ \ell(F)=\min\{i:b_F\in Z_i(x)\},
22
+ \qquad Z_{-1}(x)=\varnothing.
23
+ \]
24
+ All $Z_i(x)$ are subcomplexes of $T_0(x)$, so $b_F\in Z_i(x)$
25
+ is equivalent to $F\subseteq Z_i(x)$. Let $U_F$ be the connected
26
+ component of $Z_{\ell(F)}(x)\setminus Z_{\ell(F)-1}(x)$ containing
27
+ $b_F$. For any such component $U$, set
28
+ \begin{equation}\label{eq:component-average}
29
+ J_U=\bigcup_{p\in U}\supp p,
30
+ \qquad
31
+ u_U=\frac{1}{|J_U|}\sum_{v\in J_U}\delta_v.
32
+ \end{equation}
33
+ The next lemma proves that $J_U$ is finite and controls these
34
+ labels as $x$ varies. The intended image of an oriented barycentric
35
+ simplex is
36
+ \begin{equation}\label{eq:exterior-replacement}
37
+ [b_{F_0},\ldots,b_{F_j}]
38
+ \longmapsto u_{U_{F_0}}\wedge\cdots\wedge u_{U_{F_j}}\in E_j.
39
+ \end{equation}
40
+
41
+ This choice uses the separating filtration in a specific way.
42
+ If nested faces $F\subset F'$ have the same level $i$, the segment
43
+ joining their barycenters lies in $Z_i\setminus Z_{i-1}$.
44
+ Except at its endpoint $b_F$, it lies in the relative interior
45
+ of $F'$, which the subcomplex $Z_{i-1}$ misses; the endpoint also
46
+ avoids $Z_{i-1}$ by its level. The two barycenters therefore receive
47
+ the same component vector, making any exterior term containing
48
+ both zero. Along a complete flag $F_0\subset\cdots\subset F_n$,
49
+ with $\dim F_i=i$, the levels are nondecreasing: if
50
+ $F\subset F'\subseteq Z_i$, then $F\subseteq Z_i$.
51
+ A nonzero image must consequently use all levels $0,1,\ldots,n$,
52
+ beginning at a point of $Z_0$. We will bound the number of these
53
+ flags after establishing that the labels define finite chains.
54
+
55
+ \begin{lemma}\label{lem:finite-component-labels}
56
+ For every original simplex $\kappa$ of $K$, there is a finite set
57
+ $W_\kappa\subseteq Y$, independent of $\epsilon$ and $x$, such that
58
+ $J_{U_F}\subseteq W_\kappa$ whenever $b_F\in\kappa$. The triangulation
59
+ over $\kappa$, together with all its assigned vectors $u_{U_F}$,
60
+ is locally constant in $x$. These assignments are equivariant.
61
+ \end{lemma}
62
+
63
+ \begin{proof}
64
+ Each component of $Z_i(x)\setminus Z_{i-1}(x)$ has
65
+ $\rho$-diameter at most $2R$. For $i=0$ the components are
66
+ singletons, since $Z_0(x)$ is a locally finite zero-dimensional
67
+ subcomplex. If $b_F\in\kappa$ and $p\in U_F$, the support-distance
68
+ bound from Lemma~\ref{lem:proper} gives
69
+ \[
70
+ \min d_Y(\supp b_F,\supp p)
71
+ \leq\sqrt n\,\rho(b_F,p)\leq 2R\sqrt n.
72
+ \]
73
+ Choose an original top simplex containing $p$. Its $n+1$ vertices
74
+ span a connected graph, so every vertex in $\supp p$ is within
75
+ graph distance $n$ of the vertex furnished by this inequality.
76
+ Consequently we may take
77
+ \[
78
+ W_\kappa=
79
+ \left\{v\in Y:
80
+ d_Y\bigl(v,V(\kappa)\bigr)
81
+ \leq\left\lceil 2R\sqrt n+n\right\rceil\right\}.
82
+ \]
83
+ The bounded degree of $Y$ makes this set finite. Notice that the
84
+ support of $p$ need not itself span a connected graph; we used
85
+ the containing top simplex.
86
+
87
+ Let $K[W_\kappa]$ be the finite subcomplex consisting of the simplices
88
+ whose vertices belong to $W_\kappa$. The whole component $U_F$
89
+ lies in its realization. It follows that $U_F$ is exactly the
90
+ component containing $b_F$ in
91
+ \[
92
+ \bigl(Z_{\ell(F)}(x)\setminus Z_{\ell(F)-1}(x)\bigr)
93
+ \cap |K[W_\kappa]|.
94
+ \]
95
+ Indeed $U_F$ is a connected subset of this restriction, and every
96
+ connected subset of the restriction containing $b_F$ also lies in
97
+ the original component. Thus restricting to this finite subcomplex
98
+ does not cut off a part of the component needed to compute $J_{U_F}$.
99
+
100
+ There are finitely many original simplices in $K[W_\kappa]$.
101
+ A common refinement of their finite clopen parameter partitions
102
+ makes all their triangulation and filtration data constant.
103
+ On each resulting piece the components and their sets of support
104
+ vertices are constant as well. This proves local constancy of
105
+ the assignments over $\kappa$. Finally,
106
+ $J_{hU}=hJ_U$, and hence $u_{hU}=h u_U$, proving equivariance.
107
+ \end{proof}
108
+
109
+ Subdivide each oriented original simplex into its fundamental
110
+ subdivision chain and apply the exterior assignment
111
+ \eqref{eq:exterior-replacement} to every term. This defines a map
112
+ $f_x:C_*(K)\to E_*$. Both operations commute
113
+ with the augmented boundary. For subdivision, interior facets
114
+ cancel in pairs and the boundary facets give the compatible
115
+ subdivision on each original face. For the second operation,
116
+ each assigned vector has coefficient sum one, so contraction
117
+ with the coefficient-sum functional gives
118
+ \[
119
+ \partial(u_0\wedge\cdots\wedge u_j)
120
+ =\sum_{i=0}^j(-1)^i
121
+ u_0\wedge\cdots\wedge\widehat{u_i}\wedge\cdots\wedge u_j.
122
+ \]
123
+ Thus $f_x$ is an augmented chain map.
124
+
125
+ By Lemma~\ref{lem:finite-component-labels}, its value on any
126
+ original simplex is constant on a finite clopen partition and
127
+ is supported in a fixed finite exterior space. We may therefore
128
+ define
129
+ \begin{equation}\label{eq:averaged-chain-map}
130
+ F^\epsilon(c)=\int_X f_x(c)\,d\mu(x).
131
+ \end{equation}
132
+ This integral is an actual finite chain: for every $c$ it is a
133
+ finite linear combination of finitely many chain values.
134
+ It commutes with the augmented boundary. Moreover,
135
+ $f_{hx}(hc)=h f_x(c)$, so invariance of $\mu$ shows that
136
+ $F^\epsilon$ is $H$-equivariant.
137
+
138
+ \subsection{Counting the surviving flags}
139
+
140
+ We now bound the evaluation of $f_x$ on a top simplex. The number
141
+ of subdivision simplices may depend on $\epsilon$; the following
142
+ bound depends instead on the number of zero-stratum points.
143
+ The component-labeling and flag-counting method is modeled on
144
+ Alpert \cite[Lemmas 4 and 10]{Alpert2025}; the carrier argument below
145
+ supplies the bound without a manifold hypothesis.
146
+
147
+ \begin{lemma}\label{lem:surviving-flags}
148
+ For every original top simplex $\sigma$ and every $x$, at most
149
+ \[
150
+ 2^n\#\bigl(Z_0(x)\cap\sigma\bigr)
151
+ \]
152
+ terms in its fundamental barycentric subdivision chain have
153
+ nonzero images under the exterior replacement map.
154
+ \end{lemma}
155
+
156
+ \begin{proof}
157
+ Suppress $x$. Such a term corresponds to a complete flag
158
+ \[
159
+ F_0\subset F_1\subset\cdots\subset F_n,
160
+ \qquad \dim F_i=i,
161
+ \]
162
+ in the restriction of $T_0$ to $\sigma$. As shown when defining
163
+ \eqref{eq:exterior-replacement}, a nonzero term has levels exactly
164
+ $0,1,\ldots,n$. In particular $F_0=\{z\}$ for a point
165
+ $z\in Z_0\cap\sigma$ and $F_i\subseteq Z_i$ for every $i$.
166
+
167
+ By Lemma~\ref{lem:carrier}, $z$ lies in the relative interior of
168
+ a unique $i$-simplex $S_i$ of $T_i$ contained in $Z_i$. To see why
169
+ this carrier controls the final refinement, let $F_i$ occur in a
170
+ surviving flag through $z$. The $T_i$-carrier of a relative-interior
171
+ point of $F_i$ contains $F_i$ by refinement and belongs to $Z_i$,
172
+ because $Z_i$ is a subcomplex. That carrier has dimension at least
173
+ $i$, since it contains $F_i$, and at most $i$, since $\dim Z_i\leq i$.
174
+ It contains $z$, so it equals $S_i$. Hence $F_i\subseteq S_i$.
175
+
176
+ For a fixed preceding face $F_{i-1}$, the possible $F_i$ are thus
177
+ full-dimensional simplices in a triangulation of the single affine
178
+ $i$-simplex $S_i$, having $F_{i-1}$ as a facet. There is at most one
179
+ on either side of the affine hyperplane spanned by that facet.
180
+ Otherwise two simplices on the same side would have intersecting
181
+ relative interiors near an interior point of the facet. There
182
+ are therefore at most two choices at each stage and at most $2^n$
183
+ surviving flags through $z$. Summing over $z$ proves the assertion.
184
+ This argument concerns one carrier simplex at a time and uses no
185
+ manifold assumption on $K$ or on the strata.
186
+ \end{proof}
187
+
188
+ Figure~\ref{fig:flags} illustrates the two choices at each of the two
189
+ stages when $n=2$.
190
+
191
+ \begin{figure}[htbp]
192
+ \centering
193
+ \begin{tikzpicture}[scale=1.05]
194
+ \coordinate (A) at (-2,0);
195
+ \coordinate (B) at (2,0);
196
+ \coordinate (C) at (0,3);
197
+ \coordinate (L) at (-1.3333,1);
198
+ \coordinate (R) at (1.3333,1);
199
+ \coordinate (z) at (0,1);
200
+ \fill[blue!9] (L)--(z)--(C)--cycle;
201
+ \fill[blue!18] (z)--(R)--(C)--cycle;
202
+ \fill[orange!13] (L)--(z)--(A)--cycle;
203
+ \fill[orange!24] (z)--(R)--(A)--cycle;
204
+ \draw[thin,gray] (z)--(A) (A)--(R) (z)--(C);
205
+ \draw[thick] (A)--(B)--(C)--cycle;
206
+ \draw[very thick,blue!65!black] (L)--(R);
207
+ \fill (z) circle (2pt) node[below right=2pt,fill=white,inner sep=1pt] {$z$};
208
+ \node at (-0.44,1.68) {$F_2$};
209
+ \node at (0.44,1.68) {$F_2$};
210
+ \node at (-1.08,0.62) {$F_2$};
211
+ \node at (-0.25,0.67) {$F_2$};
212
+ \node[above=2pt] at (-0.66,1) {$F_1$};
213
+ \node[above=2pt] at (0.66,1) {$F_1$};
214
+ \end{tikzpicture}
215
+ \caption{The flag count in dimension two. The point $z\in Z_0$ has
216
+ two possible incident edges $F_1$ along its one-dimensional carrier.
217
+ Each edge has at most two incident triangles $F_2$ inside the original
218
+ two-dimensional carrier. The four shaded triangles give the four possible
219
+ flags through $z$ in this example. The unshaded triangle has no
220
+ one-dimensional-stratum edge through $z$.}
221
+ \label{fig:flags}
222
+ \end{figure}
223
+
224
+ Let $\psi:E_n\to\C$ be the invariant cocycle in
225
+ Theorem~\ref{thm:sparse}. For an original top simplex $\sigma$, put
226
+ \[
227
+ M_\sigma=
228
+ \max_{v_0,\ldots,v_n\in W_\sigma}
229
+ \left|\psi(\delta_{v_0}\wedge\cdots\wedge\delta_{v_n})\right|.
230
+ \]
231
+ This is finite, even though $\psi$ need not be bounded on all
232
+ basis simplices of the infinite vertex set. Every vector in
233
+ \eqref{eq:component-average} is a nonnegative convex combination
234
+ of vertices in $W_\sigma$. Multilinearity therefore bounds the
235
+ evaluation of each surviving term by $M_\sigma$. The preceding
236
+ lemma and Proposition~\ref{prop:zero-strata} give
237
+ \begin{align}
238
+ \left|\psi\bigl(F^\epsilon(\sigma)\bigr)\right|
239
+ &\leq 2^n M_\sigma
240
+ \int_X\#\bigl(Z_0(x)\cap\sigma\bigr)\,d\mu(x)
241
+ \notag\\
242
+ &\leq 2^n M_\sigma C_\sigma\epsilon
243
+ \longrightarrow 0.\label{eq:small-chain-evaluation}
244
+ \end{align}
245
+ All constants here are independent of $\epsilon$. Since chains
246
+ have finite support, the same convergence holds on every fixed
247
+ $c\in C_n(K)$.
248
+
249
+ \subsection{Equivariant comparison and passage to coinvariants}
250
+
251
+ It remains to show that the small evaluations just obtained equal
252
+ the original cocycle evaluation on every coinvariant cycle.
253
+ We do this by constructing a homotopy before taking coinvariants.
254
+
255
+ \begin{lemma}\label{lem:equivariant-homotopy}
256
+ Let $K$ be a simplicial complex with an $H$-action and finite
257
+ setwise simplex stabilizers. Let $E_*$ be the augmented exterior
258
+ chain complex on a nonempty $H$-set. Any two $H$-equivariant
259
+ augmented chain maps $A,B:C_*(K)\to E_*$ that agree in degree $-1$
260
+ are $H$-equivariantly chain homotopic.
261
+ \end{lemma}
262
+
263
+ \begin{proof}
264
+ The target is acyclic as an augmented complex. Indeed, for any
265
+ fixed vertex $v$, the operator $a\mapsto\delta_v\wedge a$ satisfies
266
+ \[
267
+ \partial(\delta_v\wedge a)+\delta_v\wedge\partial a=a.
268
+ \]
269
+ This contraction need not be equivariant. We use it only to choose
270
+ finite fillers and then impose equivariance by finite averaging.
271
+
272
+ Set $h_{-1}=0$. Suppose the homotopy has been constructed below
273
+ degree $j$. For an oriented $j$-simplex $e$, the residual
274
+ \[
275
+ r(e)=A(e)-B(e)-h_{j-1}(\partial e)
276
+ \]
277
+ is a cycle, by the chain-map identities and the previously
278
+ constructed homotopy. Choose a finite chain $t$ with
279
+ $\partial t=r(e)$. Let $S$ be the setwise stabilizer of $e$ and
280
+ let $\chi:S\to\{1,-1\}$ be its orientation character, so that
281
+ $s e=\chi(s)e$. The residual is equivariant, and hence
282
+ $s r(e)=\chi(s)r(e)$. Define
283
+ \[
284
+ \overline t=\frac1{|S|}\sum_{s\in S}\chi(s)\,s t.
285
+ \]
286
+ Then $\partial\overline t=r(e)$ and
287
+ $s\overline t=\chi(s)\overline t$. Choose such a filler for one
288
+ oriented representative of every simplex orbit, put
289
+ $h_j(e)=\overline t$, and extend equivariantly and linearly.
290
+ The orientation-character identity makes the extension
291
+ well-defined, including when the stabilizer reverses orientation.
292
+ This gives $A-B=\partial h+h\partial$ in degree $j$ and completes
293
+ the induction.
294
+ \end{proof}
295
+
296
+ \begin{proof}[Proof of Theorem~\ref{thm:sparse}]
297
+ The geometric construction applies for every sufficiently large
298
+ $n$ depending only on $D$, as fixed by \eqref{eq:strict-volume}.
299
+ For nonempty $K$, construct $F^\epsilon$ as above. The stabilizers
300
+ are finite by Lemma~\ref{lem:proper}, and $F^\epsilon$ and inclusion
301
+ $\iota$ both induce the identity in augmented degree $-1$.
302
+ Lemma~\ref{lem:equivariant-homotopy} supplies an equivariant
303
+ homotopy
304
+ \[
305
+ \iota-F^\epsilon=\partial h+h\partial.
306
+ \]
307
+
308
+ Let $\overline c$ be a cycle of $C_n(K)_H$ and choose a finite
309
+ chain lift $c\in C_n(K)$. We do not assume that $c$ is a cycle
310
+ before taking coinvariants. Its boundary is a finite sum of
311
+ differences $ha-a$. Equivariance of the homotopy makes
312
+ $h_{n-1}(\partial c)$ another such sum, which the invariant
313
+ functional $\psi$ annihilates. The cocycle identity annihilates
314
+ $\partial h_n(c)$. Thus, for every $\epsilon>0$,
315
+ \[
316
+ \psi\bigl(\iota(c)\bigr)
317
+ =\psi\bigl(F^\epsilon(c)\bigr).
318
+ \]
319
+ The right-hand side tends to zero by
320
+ \eqref{eq:small-chain-evaluation}, whereas the left-hand side
321
+ does not depend on $\epsilon$. Hence it is zero. The evaluation
322
+ depends only on the coinvariant class because $\psi$ is invariant.
323
+ For empty $K$ there is no nonzero top chain to consider.
324
+ \end{proof}
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/07-idempotents.tex ADDED
@@ -0,0 +1,258 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Cycles from an idempotent}
2
+ \label{sec:idempotents}
3
+
4
+ We now return to group rings. For an idempotent and one infinite-order
5
+ conjugacy class, we will construct cycles in every positive even degree.
6
+ Their vertices follow steps in one fixed graph of bounded degree. In
7
+ sufficiently high dimension, the supporting complexes will therefore
8
+ satisfy the hypotheses of Theorem~\ref{thm:sparse}. We first record why
9
+ it suffices to perform this construction for finitely generated groups.
10
+
11
+ The use of cyclic idempotent expressions and reduced centralizers has
12
+ its conceptual background in Connes's pairing with projective classes
13
+ \cite[Part II, Section 2, Proposition 14]{Connes1985} and Burghelea's
14
+ conjugacy-class decomposition \cite[Theorem I]{Burghelea1985}. Our finite
15
+ path identities and the detector's normalization are proved directly;
16
+ no cyclic-homology identification is assumed.
17
+
18
+ \begin{lemma}[Subgroup locality]\label{lem:locality}
19
+ Let $i:L\hookrightarrow G$ be an inclusion of discrete groups. Extension
20
+ of scalars defines $i_*:K_0(\C L)\to K_0(\C G)$, and for every
21
+ $y\in K_0(\C L)$ and $C\in\con(G)$,
22
+ \begin{equation}\label{eq:class-aggregation}
23
+ \HS_G(i_*y)(C)
24
+ =\sum_{\substack{B\in\con(L)\\ B\subseteq L\cap C}}
25
+ \HS_L(y)(B).
26
+ \end{equation}
27
+ Only finitely many terms are nonzero. Moreover, every
28
+ $x\in K_0(\C G)$ is induced from a finitely generated subgroup, which may
29
+ be required to contain any prescribed finite subset of $G$.
30
+ Consequently, the finite-order-support assertion of
31
+ Theorem~\ref{thm:bass} for all finitely generated groups implies that
32
+ assertion for all discrete groups.
33
+ \end{lemma}
34
+
35
+ \begin{proof}
36
+ We regard free right modules as columns: an idempotent
37
+ $e\in M_r(\C L)$ acts on the left, with image $e(\C L)^r$.
38
+ Tensoring the split decomposition defined by $e$ with $\C G$ identifies
39
+ the extended image with $e(\C G)^r$. The coefficient sum in an ambient
40
+ class $C$ is the sum of its coefficient sums over all $L$-classes contained
41
+ in $L\cap C$. This proves \eqref{eq:class-aggregation} for the image of an
42
+ idempotent and then, by subtraction, for every virtual class. Finiteness
43
+ follows from the finite coefficient support of the matrices representing
44
+ that class.
45
+
46
+ Write an arbitrary $x\in K_0(\C G)$ as the difference of the classes of
47
+ two finite idempotent matrices. The group generated by their coefficient
48
+ supports and the prescribed finite subset is finitely generated. The
49
+ same matrices are idempotent over its group ring, since that ring embeds
50
+ in $\C G$, and their difference induces $x$. Finally, if an ambient class
51
+ consists of infinite-order elements, so does every subgroup class occurring
52
+ in \eqref{eq:class-aggregation}: subgroup inclusion preserves the order of
53
+ an element. Vanishing of each subgroup coefficient therefore gives
54
+ vanishing of the ambient coefficient. This uses all the subgroup classes
55
+ in the sum, since an ambient conjugacy class can split into several of
56
+ them.
57
+ \end{proof}
58
+
59
+ \subsection{A fixed graph and finite path sums}
60
+
61
+ For the rest of this section, fix a finitely generated group $G$, an
62
+ idempotent $e\in M_r(\C G)$, and an infinite-order element $g\in G$.
63
+ Write
64
+ \[
65
+ e=\sum_{s\in G}A_s s,\qquad A_s\in M_r(\C),\qquad
66
+ S_0=\{s\in G:A_s\ne0\}.
67
+ \]
68
+ The set $S_0$ is finite. Idempotence says that
69
+ $\sum_{uv=t}A_uA_v=A_t$ for every $t\in G$. Thus the matrix-valued kernel
70
+ \[
71
+ a(h,h')=A_{h^{-1}h'}
72
+ \]
73
+ is invariant under simultaneous left translation and satisfies
74
+ \begin{equation}\label{eq:kernel-idempotence}
75
+ \sum_{k\in G}a(h,k)a(k,h')
76
+ =\sum_{uv=h^{-1}h'}A_uA_v
77
+ =a(h,h').
78
+ \end{equation}
79
+ All these sums are finite. In particular, the order of the matrix
80
+ factors agrees with the column convention for right modules.
81
+
82
+ Put
83
+ \[
84
+ J=C_G(g),\qquad H=J/\langle g\rangle,\qquad
85
+ Y=\langle g\rangle\backslash G,
86
+ \qquad \bar h=\langle g\rangle h.
87
+ \]
88
+ Choose a finite symmetric generating set $S\subset G\setminus\{1\}$
89
+ containing $S_0\setminus\{1\}$ and its inverses. Give $Y$ the simple
90
+ undirected graph whose edges join $\bar h$ to $\overline{hs}$ for $s\in S$;
91
+ loops are omitted and repeated edges identified. The graph is connected
92
+ and has degree at most the fixed integer
93
+ \[
94
+ D=\max\{2,|S|\}.
95
+ \]
96
+ The group $H$ acts by left multiplication. This is well-defined because
97
+ $J$ centralizes $g$, and it preserves right-step edges. It is free on
98
+ vertices: $\overline{ch}=\bar h$ with $c\in J$ implies $ch=g^q h$ for an
99
+ integer $q$, and hence $c=g^q$. Both $H$ and $Y$ are countable. We keep
100
+ this graph and this value of $D$ throughout all subsequent choices of
101
+ dimension.
102
+
103
+ For $k\ge1$, let $Q_k=J\backslash G^k$, with simultaneous left
104
+ translation on tuples. Define the weight of a tuple by
105
+ \begin{equation}\label{eq:path-weight}
106
+ w_k(h_0,\ldots,h_{k-1})
107
+ =\tr\bigl(a(h_0,h_1)\cdots
108
+ a(h_{k-2},h_{k-1})a(h_{k-1},gh_0)\bigr),
109
+ \end{equation}
110
+ where $w_1(h_0)=\tr(a(h_0,gh_0))$. These weights are $J$-invariant.
111
+ They define a finite complex linear combination $v_k$ of elements of
112
+ $Q_k$. Indeed, a nonzero weight has increments
113
+ \[
114
+ s_i=h_i^{-1}h_{i+1}\quad(0\le i<k-1),\qquad
115
+ s_{k-1}=h_{k-1}^{-1}gh_0
116
+ \]
117
+ in $S_0$, with
118
+ \[
119
+ s_0\cdots s_{k-1}=h_0^{-1}gh_0.
120
+ \]
121
+ An increment list determines the tuple from $h_0$. Any two choices of
122
+ $h_0$ with this conjugate differ by left multiplication in $J$, so the
123
+ list determines at most one element of $Q_k$. Hence $v_k$ has at most
124
+ $|S_0|^k$ nonzero coefficients. For a $J$-invariant function $p$ on
125
+ $G^k$, write $v_k(p)$ for the finite weighted sum of its values. These
126
+ weights need not be real or positive.
127
+
128
+ \begin{lemma}[Path identities]\label{lem:path-identities}
129
+ For the path sums associated to $e$ and $g$, the twisted cyclic shift
130
+ \[
131
+ T(h_0,\ldots,h_{k-1})=(h_1,\ldots,h_{k-1},gh_0)
132
+ \]
133
+ preserves $v_k$. For $k\ge2$, deletion of any entry induces a map
134
+ $d_i:Q_k\to Q_{k-1}$ satisfying
135
+ \[
136
+ (d_i)_*v_k=v_{k-1}\qquad(0\le i<k).
137
+ \]
138
+ Every $v_k$ has the same total weight
139
+ \begin{equation}\label{eq:trace-coefficient}
140
+ \lambda:=v_k(1)
141
+ =\sum_{s\in[g]_G}\tr(A_s)
142
+ =\HS_G\bigl([e(\C G)^r]\bigr)([g]_G).
143
+ \end{equation}
144
+ \end{lemma}
145
+
146
+ \begin{proof}
147
+ The shift $T$ is a $J$-equivariant bijection, with inverse
148
+ \[
149
+ (h_0,\ldots,h_{k-1})\longmapsto
150
+ (g^{-1}h_{k-1},h_0,\ldots,h_{k-2}).
151
+ \]
152
+ For $k=1$, the shift is the identity on $Q_1$, since $g\in J$.
153
+ For $k\ge2$, the shifted weight has the factors of
154
+ \eqref{eq:path-weight} in cyclic order, since
155
+ $a(gh_0,gh_1)=a(h_0,h_1)$. Cyclicity of the matrix trace proves
156
+ $T_*v_k=v_k$.
157
+
158
+ For deletion, fix a representative of the shorter tuple. Each orbit in
159
+ its fibre has a unique representative with exactly those retained
160
+ entries, because simultaneous left translation acts freely on any
161
+ nonempty tuple. Thus the fibre sum is over the missing entry in $G$,
162
+ without a stabilizer factor. Internal deletions follow from
163
+ \eqref{eq:kernel-idempotence}, as does deletion of the last entry using
164
+ \[
165
+ \sum_u a(h_{k-2},u)a(u,gh_0)=a(h_{k-2},gh_0).
166
+ \]
167
+ For the first deletion, fix $(h_1,\ldots,h_{k-1})$ and put
168
+ $B=a(h_1,h_2)\cdots a(h_{k-2},h_{k-1})$, with $B=I_r$ when $k=2$.
169
+ Then
170
+ \begin{align*}
171
+ &\sum_{h_0}\tr\bigl(a(h_0,h_1)B a(h_{k-1},gh_0)\bigr)\\
172
+ &\qquad=\sum_{h_0}\tr\bigl(Ba(h_{k-1},gh_0)a(gh_0,gh_1)\bigr)\\
173
+ &\qquad=\tr\bigl(Ba(h_{k-1},gh_1)\bigr).
174
+ \end{align*}
175
+ Here the first equality uses trace cyclicity and left invariance; the
176
+ second uses \eqref{eq:kernel-idempotence} with the substitution $u=gh_0$.
177
+ This also proves the assertion for $k=2$. The kernel has finite row and
178
+ column support, so every fibre sum used in these computations is finite.
179
+
180
+ The deletion identities show that all total weights equal $v_1(1)$.
181
+ Finally,
182
+ \[
183
+ J\backslash G\longrightarrow[g]_G,\qquad Jh\longmapsto h^{-1}gh
184
+ \]
185
+ is a bijection: equality of the conjugates is equivalent to
186
+ $h'h^{-1}\in J$. Therefore
187
+ $v_1(1)=\sum_{s\in[g]_G}\tr(A_s)$, which is precisely the indicated
188
+ Hattori--Stallings coefficient.
189
+ \end{proof}
190
+
191
+ \subsection{Even-dimensional cycles}
192
+
193
+ The path identities now turn the finite sums into cycles. We use the
194
+ exterior complex $E_*$ on the graph $Y$.
195
+ For $k\ge1$, define
196
+ \[
197
+ \pi_k:\C^{(Q_k)}\longrightarrow(E_{k-1})_H,\qquad
198
+ [h_0,\ldots,h_{k-1}]\longmapsto
199
+ [\delta_{\bar h_0}\wedge\cdots\wedge\delta_{\bar h_{k-1}}].
200
+ \]
201
+ The map is well-defined because changing a tuple by an element of $J$
202
+ changes its projected vertices by a simultaneous $H$-translation.
203
+ Set $b_k=\pi_k(v_k)$, and, for $n=2m\ge2$, set
204
+ \[
205
+ z_n=b_{n+1}\in(E_n)_H.
206
+ \]
207
+
208
+ \begin{proposition}\label{prop:path-cycle}
209
+ For every positive even integer $n$, the chain $z_n$ is a cycle.
210
+ Moreover, either its defining sum has no nonzero distinct-vertex terms,
211
+ so $z_n=0$, or it is the image of a cycle in $C_n(K)_H$ for an
212
+ $H$-invariant simplicial complex $K$ generated by $n$-simplices, with
213
+ finitely many simplex orbits, whose top vertex sets span connected
214
+ subgraphs of $Y$. The graph and its degree bound $D$ are independent
215
+ of $n$.
216
+ \end{proposition}
217
+
218
+ \begin{proof}
219
+ Since $\overline{gh_0}=\bar h_0$, the twisted shift projects to the cyclic
220
+ permutation of the $k$ wedge factors. Hence
221
+ \[
222
+ \pi_kT=(-1)^{k-1}\pi_k.
223
+ \]
224
+ Together with $T_*v_k=v_k$, this shows that $b_k=0$ whenever $k$ is even.
225
+ The deletion identities give
226
+ \[
227
+ \partial b_k=\sum_{i=0}^{k-1}(-1)^i b_{k-1}\qquad(k\ge2).
228
+ \]
229
+ For even $n$, it follows that $\partial z_n=b_n=0$.
230
+
231
+ A tuple with repeated projected vertices contributes zero to the wedge.
232
+ For every remaining tuple with nonzero weight, consecutive projected
233
+ vertices are joined by edges from the fixed step set $S$. Their path
234
+ visits all its $n+1$ vertices, so the subgraph spanned by those vertices
235
+ is connected. Let $K$ be generated by these vertex sets and their
236
+ $H$-translates. Finite support of $v_{n+1}$ gives finitely many orbits
237
+ of top simplices and of their faces.
238
+
239
+ The same finite expression for $z_n$ defines a chain in $C_n(K)_H$.
240
+ To see that its boundary is zero there, decompose $E_j$ in every degree
241
+ as the direct sum of the span of the oriented simplices belonging to
242
+ $K$ and the span of all other oriented simplices. Both summands are
243
+ $H$-invariant, including their orientation signs. Thus
244
+ \[
245
+ E_j=C_j(K)\oplus W_j,
246
+ \qquad
247
+ (E_j)_H=C_j(K)_H\oplus(W_j)_H.
248
+ \]
249
+ In particular the inclusion remains injective after taking
250
+ coinvariants. The boundary of the chain in $C_n(K)_H$ maps to
251
+ $\partial z_n=0$, so it is zero already in $C_{n-1}(K)_H$.
252
+ \end{proof}
253
+
254
+ We have obtained the required sparse cycles in arbitrarily large even
255
+ degrees. The underlying path sums all have total weight $\lambda$, the trace
256
+ coefficient in \eqref{eq:trace-coefficient}. The next section constructs
257
+ a cocycle whose value on $z_{2m}$ recovers a nonzero scalar multiple of
258
+ that coefficient.
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/08-detector.tex ADDED
@@ -0,0 +1,203 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A Pfaffian cocycle detecting the trace coefficient}
2
+ \label{sec:detector}
3
+
4
+ Retain the finitely generated group $G$, idempotent, infinite-order element
5
+ $g$, and notation $J,H,Y,v_k,\lambda,z_{2m}$ of
6
+ Section~\ref{sec:idempotents}. We construct an $H$-invariant cocycle whose
7
+ value on $z_{2m}$ is $2^{-m}\lambda$. The construction first records the
8
+ relative powers of $g$ between two lifts of vertices of $Y$. An alternating
9
+ Pfaffian expression will then remove the dependence on those lifts.
10
+
11
+ \subsection{Relative exponents between lifts}
12
+
13
+ \begin{lemma}\label{lem:beta}
14
+ There is a $J$-invariant function $\beta:G\times G\to\R$ such that
15
+ \begin{equation}\label{eq:beta-properties}
16
+ \beta(h',h)=-\beta(h,h'),\qquad
17
+ \beta(g^r h,g^s h')=\beta(h,h')+s-r
18
+ \quad(r,s\in\Z).
19
+ \end{equation}
20
+ \end{lemma}
21
+
22
+ \begin{proof}
23
+ The diagonal $H$-action on the set of ordered pairs $Y\times Y$ is free,
24
+ because its action on the first coordinate is free. This also applies to
25
+ diagonal pairs $(y,y)$. For each orbit choose a representative $(y_o,y'_o)$
26
+ and lifts $(l_o,l'_o)\in G^2$. For $(h,h')\in G^2$, there is a unique
27
+ $\bar c\in H$ carrying the appropriate representative to the projected
28
+ pair. Choose a lift $c\in J$ and write
29
+ \[
30
+ h=g^r c l_o,\qquad h'=g^s c l'_o.
31
+ \]
32
+ For fixed $c$, the integers $r,s$ are unique because $g$ has infinite order.
33
+ Replacing $c$ by $g^t c$ replaces them by $r-t,s-t$. Thus
34
+ $B(h,h')=s-r$ is well defined. Commutation with $g$ shows that $B$ is
35
+ $J$-invariant, and independently changing the two lifts gives
36
+ \[
37
+ B(g^a h,g^b h')=B(h,h')+b-a.
38
+ \]
39
+ The antisymmetrization
40
+ \[
41
+ \beta(h,h')=\frac{B(h,h')-B(h',h)}2
42
+ \]
43
+ has all the required properties.
44
+ \end{proof}
45
+
46
+ The function $\beta$ itself need not descend to $Y\times Y$. In fact,
47
+ \eqref{eq:beta-properties} gives $\beta(h,g^k h)=k$ even though these two
48
+ lifts project to the same vertex. Nor is there a difficulty if an element
49
+ $\bar c\in H$ exchanges two distinct projected vertices. If a lift
50
+ $c\in J$ satisfies
51
+ $c h_0=g^a h_1$ and $c h_1=g^b h_0$, its invariance merely requires
52
+ \[
53
+ 2\beta(h_0,h_1)=b-a,
54
+ \]
55
+ which is precisely what antisymmetrization gives. Real values are useful
56
+ here: for $G=\langle t\rangle$ and $g=t^2$, the value
57
+ $\beta(1,t)=1/2$ is forced.
58
+
59
+ \subsection{The cyclic Pfaffian identity}
60
+
61
+ In degree two, a lift-independent expression is
62
+ \[
63
+ c(y_0,y_1,y_2)
64
+ =\beta(h_1,h_2)-\beta(h_0,h_2)+\beta(h_0,h_1),
65
+ \qquad \bar h_i=y_i.
66
+ \]
67
+ Changing $h_i$ to $g^{r_i}h_i$ adds
68
+ $(r_2-r_1)-(r_2-r_0)+(r_1-r_0)=0$, so $c$ depends only on the
69
+ projected vertices. In higher even degrees we replace $\beta$ by a
70
+ Pfaffian and take the same alternating deletion sum. The Pfaffian
71
+ still depends on the lifts; its deletion sum will define the cocycle.
72
+ We first compute the weighted Pfaffian sum, then prove the descent
73
+ and cocycle properties of its deletion sum.
74
+
75
+ For a list $\mathbf h=(h_0,\ldots,h_{2m-1})$ with $m\ge1$, let
76
+ \[
77
+ p_m(\mathbf h)=\operatorname{Pf}
78
+ \bigl(\beta(h_i,h_j)\bigr)_{0\le i,j<2m},
79
+ \qquad p_0=1.
80
+ \]
81
+ We use the convention that $p_m(\mathbf h)$ is the coefficient of
82
+ $\varepsilon_0\wedge\cdots\wedge\varepsilon_{2m-1}$ in $b^m/m!$, where
83
+ $\varepsilon_i$ are the coordinate one-forms on the space of list positions
84
+ and
85
+ \[
86
+ b=\sum_{i<j}\beta(h_i,h_j)\,
87
+ \varepsilon_i\wedge\varepsilon_j.
88
+ \]
89
+ In particular, $p_1(h_0,h_1)=\beta(h_0,h_1)$, and $p_m$ is alternating in
90
+ its entries and $J$-invariant. The finite weighted sums
91
+ \[
92
+ q_m=v_{2m}(p_m)\quad(m\ge1),\qquad q_0=\lambda
93
+ \]
94
+ are therefore defined. No boundedness of $p_m$ on all lists is needed.
95
+
96
+ \begin{lemma}\label{lem:pfaffian-recurrence}
97
+ For every $m\ge1$, one has $q_m=\tfrac12q_{m-1}$ and hence
98
+ $q_m=2^{-m}\lambda$.
99
+ \end{lemma}
100
+
101
+ \begin{proof}
102
+ An ordinary cyclic rotation of a list of length $2m$ changes its Pfaffian
103
+ by the sign $(-1)^{2m-1}=-1$. In the twisted rotation
104
+ \[
105
+ T\mathbf h=(h_1,\ldots,h_{2m-1},g h_0),
106
+ \]
107
+ replacing the last entry $h_0$ by $g h_0$ adds $1$ to every matrix entry in
108
+ the last column above the diagonal. Expansion along that column gives
109
+ \begin{equation}\label{eq:pfaffian-rotation}
110
+ \begin{split}
111
+ p_m(T\mathbf h)
112
+ ={}&-p_m(\mathbf h)\\
113
+ &+\sum_{i=1}^{2m-1}(-1)^{i+1}
114
+ p_{m-1}(h_1,\ldots,\widehat{h_i},\ldots,h_{2m-1}).
115
+ \end{split}
116
+ \end{equation}
117
+ Indeed the last-column cofactor in position $i$, with positions numbered
118
+ $1,\ldots,2m$, has sign $(-1)^{i+1}$; each Pfaffian matching uses exactly
119
+ one entry from that column.
120
+
121
+ For $m\ge2$, each minor on the second line omits $h_0$ and $h_i$ from the
122
+ original list. Applying the deletion identity in
123
+ Lemma~\ref{lem:path-identities} twice shows that its weighted sum under
124
+ $v_{2m}$ is $q_{m-1}$. For $m=1$, the minor is $p_0=1$, whose weighted sum
125
+ is the total weight $v_2(1)=\lambda=q_0$. Thus this endpoint uses no vector
126
+ $v_0$. The invariance of $v_{2m}$ under $T$ and
127
+ $\sum_{i=1}^{2m-1}(-1)^{i+1}=1$ now turn
128
+ \eqref{eq:pfaffian-rotation} into
129
+ \[
130
+ q_m=-q_m+q_{m-1}.
131
+ \]
132
+ The claimed formulas follow.
133
+ \end{proof}
134
+
135
+ \subsection{Descent to an exterior cocycle}
136
+
137
+ The preceding calculation detects the coefficient on lists of lifts.
138
+ We next descend it to the exterior complex on $Y$, where the sparse-chain
139
+ theorem applies.
140
+
141
+ \begin{proposition}\label{prop:detector}
142
+ For every integer $m\ge1$, the formula
143
+ \begin{equation}\label{eq:detector-formula}
144
+ \psi_m(y_0,\ldots,y_{2m})
145
+ =\sum_{i=0}^{2m}(-1)^i
146
+ p_m(h_0,\ldots,\widehat{h_i},\ldots,h_{2m}),
147
+ \end{equation}
148
+ where $h_i\in G$ is any lift of $y_i\in Y$, defines an $H$-invariant
149
+ linear functional $\psi_m:E_{2m}\to\C$ satisfying
150
+ \[
151
+ \psi_m\partial=0,\qquad
152
+ \psi_m(z_{2m})=2^{-m}\lambda.
153
+ \]
154
+ Here evaluation on the coinvariant chain $z_{2m}$ is defined by
155
+ $H$-invariance.
156
+ \end{proposition}
157
+
158
+ \begin{proof}
159
+ On the $2m+1$ list positions put
160
+ \[
161
+ u=\sum_{i=0}^{2m}\varepsilon_i,
162
+ \qquad
163
+ b=\sum_{0\le i<j\le2m}\beta(h_i,h_j)\,
164
+ \varepsilon_i\wedge\varepsilon_j.
165
+ \]
166
+ The right side of \eqref{eq:detector-formula} is the coefficient of the
167
+ ordered top form in $u\wedge b^m/m!$. Moving the factor
168
+ $\varepsilon_i$ past its $i$ preceding positions gives exactly the sign
169
+ $(-1)^i$ in that formula.
170
+
171
+ Changing the lifts to $g^{r_i}h_i$ replaces $\beta(h_i,h_j)$ by
172
+ $\beta(h_i,h_j)+r_j-r_i$. Thus it replaces $b$ by
173
+ $b+u\wedge v$, with $v=\sum_i r_i\varepsilon_i$. Every correction term
174
+ in $u\wedge(b+u\wedge v)^m$ contains two factors $u$ and vanishes.
175
+ This proves independence of the lifts.
176
+
177
+ The expression is alternating in the lifted list. After lift independence
178
+ has been established, it is therefore alternating in the projected
179
+ vertices as well. In particular, if two projected vertices coincide,
180
+ choose equal lifts for them to see that the expression vanishes. It
181
+ consequently defines a linear functional on
182
+ $E_{2m}=\bigwedge^{2m+1}\C^{(Y)}$.
183
+ For $\bar c\in H$, choose $c\in J$ and use $c h_i$ as the lifts of the
184
+ translated vertices. The $J$-invariance of $\beta$ proves the
185
+ $H$-invariance of $\psi_m$.
186
+
187
+ To check the cocycle identity, choose lifts simultaneously for a list of
188
+ $2m+2$ vertices. On every face, \eqref{eq:detector-formula} is the
189
+ alternating deletion coboundary of $p_m$ on these same lifts. A second
190
+ deletion cancels each twice-omitted list in its two possible orders.
191
+ Hence $\psi_m\partial=0$.
192
+
193
+ Finally, $z_{2m}$ is the exterior projection of $v_{2m+1}$.
194
+ Each one-deletion term in \eqref{eq:detector-formula} has weighted sum
195
+ $v_{2m}(p_m)=q_m$, by Lemma~\ref{lem:path-identities}. Since
196
+ $\sum_{i=0}^{2m}(-1)^i=1$, their signed sum gives
197
+ \[
198
+ \psi_m(z_{2m})=q_m=2^{-m}\lambda,
199
+ \]
200
+ using Lemma~\ref{lem:pfaffian-recurrence}. Repeated projected vertices
201
+ already have zero exterior image and zero value under $\psi_m$, so they
202
+ require no separate restriction in this evaluation.
203
+ \end{proof}
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/09-completion.tex ADDED
@@ -0,0 +1,144 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Completion of the trace theorem}
2
+ \label{sec:completion}
3
+
4
+ We now combine the geometric vanishing with the detector. The order of
5
+ the choices matters: the graph is fixed by the idempotent before its
6
+ cycle dimension is chosen.
7
+
8
+ \begin{proof}[Proof of Theorem~\ref{thm:bass}]
9
+ First let $G$ be finitely generated, let $e\in M_q(\C G)$ be an
10
+ idempotent, and fix an infinite-order $g\in G$. Construct the graph on
11
+ $Y=\langle g\rangle\backslash G$ and the free action of
12
+ $H=C_G(g)/\langle g\rangle$ as in Section~\ref{sec:idempotents}.
13
+ Let $D\geq2$ be a degree bound for this fixed graph, and choose an even
14
+ integer $n=2m\geq n_0(D)$ with $m\geq1$.
15
+
16
+ Proposition~\ref{prop:path-cycle} gives the cycle $z_n$, and
17
+ Proposition~\ref{prop:detector} gives an $H$-invariant cocycle
18
+ $\psi_m:E_n\to\C$ with
19
+ \[
20
+ \psi_m(z_n)=2^{-m}\lambda,
21
+ \qquad
22
+ \lambda=\HS_G([e(\C G)^q])([g]_G).
23
+ \]
24
+ If no nonzero simplices occur, $z_n=0$ and this identity already gives
25
+ $\lambda=0$. Otherwise Proposition~\ref{prop:path-cycle} realizes $z_n$
26
+ as a cycle in $C_n(K)_H$ for an $H$-invariant complex $K$ satisfying all
27
+ hypotheses of Theorem~\ref{thm:sparse}. That theorem gives
28
+ $\psi_m(z_n)=0$, with the same conclusion. Every finitely generated
29
+ projective right $\C G$-module is represented by an idempotent, and every element of
30
+ $K_0(\C G)$ is a difference of two such classes. Additivity proves the
31
+ assertion for all finitely generated groups.
32
+
33
+ For an arbitrary discrete group $G$, choose idempotents representing
34
+ $x\in K_0(\C G)$ and let $G_0\leq G$ be generated by $g$ and all group
35
+ elements occurring in their entries. Then $G_0$ is finitely generated
36
+ and $x=i_*x_0$ for some $x_0\in K_0(\C G_0)$, where $i:G_0\hookrightarrow G$.
37
+ Lemma~\ref{lem:locality} expresses $\HS_G(x)([g]_G)$ as the sum of the
38
+ coefficients $\HS_{G_0}(x_0)(C)$ over those $G_0$-conjugacy classes
39
+ $C\subseteq G_0\cap[g]_G$. Only finitely many terms are nonzero, and
40
+ every element in every such class has infinite order. Each term
41
+ vanishes by the finitely generated case.
42
+ \end{proof}
43
+
44
+ \subsection{The integral trace}
45
+
46
+ For the integral group ring, the same idempotent formula defines
47
+ \[
48
+ \HS_{\Z G}:K_0(\Z G)\longrightarrow
49
+ \Z G/[\Z G,\Z G]\cong\bigoplus_{C\in\con(G)}\Z C,
50
+ \]
51
+ where commutators are now taken with their additive span. The integral
52
+ Bass trace conjecture asks for support only at the identity class.
53
+
54
+ \begin{corollary}\label{cor:integral}
55
+ For every discrete group $G$, the Hattori--Stallings trace of every
56
+ class in $K_0(\Z G)$ is supported on $[1]_G$.
57
+ \end{corollary}
58
+
59
+ \begin{proof}
60
+ If $P$ is a finitely generated projective right $\Z G$-module, the same
61
+ idempotent matrix over $\C G$ represents $P\otimes_{\Z G}\C G$.
62
+ Consequently its trace coefficients are the images under
63
+ $\Z\hookrightarrow\C$ of those of $P$. Theorem~\ref{thm:bass} and this
64
+ coefficientwise injection give vanishing at all infinite-order elements.
65
+ No injectivity assertion about the map between the two $K_0$ groups is
66
+ required.
67
+
68
+ For finite-order elements we use Linnell's restriction
69
+ \cite[Lemma 4.1]{Linnell1983}, in the form stated and reproved by
70
+ Berrick and Hesselholt \cite[Theorem A]{BH2015}: if the integral trace of a finitely
71
+ generated projective module is nonzero at $h$, there is an integer
72
+ $a\geq1$ such that $h$ is conjugate to $h^{s^a}$ for every integer
73
+ $s\geq1$. Their convention also uses right modules.
74
+ If $h$ has finite order $t>1$, take $s=t$.
75
+ Then $h^{t^a}=1$, so the restriction would make $h$ conjugate to $1$,
76
+ a contradiction. Thus every nonidentity finite-order coefficient also
77
+ vanishes. Taking differences of projective classes finishes the proof.
78
+ \end{proof}
79
+
80
+ \subsection{Homotopy idempotents and Lefschetz numbers}
81
+
82
+ The integral support statement also has fixed-point consequences.
83
+ A self-map $f$ is a \emph{homotopy idempotent} if $f\circ f\simeq f$.
84
+ Such a map on a connected finite CW complex $X$ admits maps
85
+ $u:X\to Y$ and $v:Y\to X$ with
86
+ \[
87
+ v\circ u\simeq f,\qquad u\circ v\simeq\id_Y
88
+ \]
89
+ \cite[Section 3]{BCM2006}. The second identity says that $Y$ is
90
+ \emph{finitely dominated} by $X$. For a pointed homotopy idempotent
91
+ with $f_\#=\id_G$, where $G=\pi_1(X)$, the induced maps $u_\#$ and
92
+ $v_\#$ identify $\pi_1(Y)$ with $G$. The universal-cover chains of $Y$
93
+ are chain homotopy equivalent to a finite complex $P_*$ of finitely
94
+ generated projective $\Z G$-modules. The sum
95
+ $\sum_i(-1)^i[P_i]\in K_0(\Z G)$ is its projective Euler class. The
96
+ Hattori--Stallings trace of this class records the fixed-point class indices of $f$:
97
+ it is the Reidemeister trace, with conjugacy classes inverted when
98
+ passing from the left-module convention of \cite[Lemma 4.1]{BCM2006}
99
+ to ours. The augmentation trace and the identity coefficient of this projective
100
+ class give the ordinary and $L^2$-Lefschetz numbers, respectively
101
+ \cite[Lemmas 8.1--8.2]{BCM2006}. Berrick, Chatterji and Mislin use these
102
+ relations to deduce the following consequences of the integral support
103
+ statement and its numerical trace consequence.
104
+
105
+ \begin{corollary}[Berrick--Chatterji--Mislin consequences]
106
+ \label{cor:homotopy-idempotents}
107
+ Let $M$ be a connected closed smooth oriented manifold.
108
+ \begin{enumerate}[label=\textup{(\roman*)}]
109
+ \item If $\dim M>2$ and $f:M\to M$ satisfies $f\circ f\simeq f$
110
+ by free homotopy, then some self-map freely homotopic to $f$ has
111
+ exactly one fixed point.
112
+ \item Choose $x_0\in M$ and put $G=\pi_1(M,x_0)$. If
113
+ $f:(M,x_0)\to(M,x_0)$ satisfies $f\circ f\simeq_* f$ by based
114
+ homotopy and $f_\#=\id_G$, then
115
+ \[
116
+ L(f)=L^{(2)}(\widetilde f).
117
+ \]
118
+ Here $\widetilde f$ is the lift to the universal cover fixing a chosen
119
+ point above $x_0$; it is $G$-equivariant. The left side is the ordinary
120
+ Lefschetz number, and the right side is the alternating sum of von
121
+ Neumann traces on the induced $L^2$-homology maps, as in
122
+ \cite[Definition 7.1]{BCM2006}.
123
+ \end{enumerate}
124
+ \end{corollary}
125
+
126
+ \begin{proof}
127
+ For $x\in K_0(\Z G)$ write $h_C(x)=\HS_{\Z G}(x)(C)$. The
128
+ augmentation trace $\epsilon$ is the sum of these coefficients, while
129
+ the Kaplansky trace $\kappa$ is the identity coefficient. The sum is
130
+ finite, and Corollary~\ref{cor:integral} gives
131
+ \[
132
+ \epsilon(x)=\sum_{C\in\con(G)}h_C(x)=h_{[1]_G}(x)=\kappa(x).
133
+ \]
134
+ This is the weak Bass conjecture for every group. The cited paper uses
135
+ projective left modules, whereas we use right modules. The anti-involution
136
+ $g\mapsto g^{-1}$, together with transpose on idempotent matrices,
137
+ transports between these conventions and relabels the coefficient at
138
+ $[g]_G$ by $[g^{-1}]_G$. It preserves identity support and both
139
+ $\epsilon$ and $\kappa$. Thus Corollary~\ref{cor:integral} gives the
140
+ classical Bass conjecture in the cited convention, and the displayed
141
+ equality gives weak Bass there. The forward implications of
142
+ \cite[Theorem 1]{BCM2006} and \cite[Theorem 2]{BCM2006} now give
143
+ \textup{(i)} and \textup{(ii)}, respectively.
144
+ \end{proof}
preprints/The-Bass-trace-conjecture-for-complex-group-rings-September-24-2026/build/sections/10-torsion-free.tex ADDED
@@ -0,0 +1,121 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Torsion-free groups: trace rank and idempotents}
2
+ \label{sec:torsion-free}
3
+
4
+ For a torsion-free group, the support theorem leaves only the identity
5
+ conjugacy class. We first identify its coefficient with augmentation
6
+ rank, and then use the two possible scalar ranks to determine scalar
7
+ idempotents.
8
+
9
+ \begin{proof}[Proof of Corollary~\ref{cor:torsion-free}\textup{(i)}]
10
+ Let $e\in M_q(\C G)$ be idempotent and put
11
+ $x=[e(\C G)^q]\in K_0(\C G)$. Since $G$ is torsion-free,
12
+ Theorem~\ref{thm:bass} says that $\HS_G(x)$ is supported on $[1]_G$.
13
+ Therefore
14
+ \begin{align}
15
+ \tau_{G,q}(e)
16
+ &=\HS_G(x)([1]_G)\notag\\
17
+ &=\sum_{C\in\con(G)}\HS_G(x)(C)\notag\\
18
+ &=\epsilon_G\!\left(\sum_{i=1}^q e_{ii}\right)
19
+ =\tr\bigl(\epsilon_{G,q}(e)\bigr)
20
+ =\operatorname{rank}_{\C}\bigl(\epsilon_{G,q}(e)\bigr).
21
+ \label{eq:torsion-free-rank}
22
+ \end{align}
23
+ The class sum is finite because the entries of $e$ have finite group
24
+ support. The last
25
+ equality holds because $\epsilon_{G,q}(e)$ is an idempotent complex
26
+ matrix: its image-kernel decomposition makes its trace equal to its
27
+ rank. Taking differences of projective classes gives
28
+ $\tau_{G,*}=\operatorname{rk}_{\epsilon}$. This map has range exactly
29
+ $\Z$, since its values are integers and $[\C G]$ has value $1$.
30
+ \end{proof}
31
+
32
+ For matrices the conclusion is numerical. For example,
33
+ $\operatorname{diag}(1,0)\in M_2(\C G)$ is an idempotent other than zero
34
+ and the identity, with augmentation rank one. The scalar case is special
35
+ because its augmentation rank can only be zero or one.
36
+
37
+ \begin{proof}[Proof of Corollary~\ref{cor:torsion-free}\textup{(ii)}]
38
+ First take $R=\C$ and let $e\in\C G$ be idempotent. Equation
39
+ \eqref{eq:torsion-free-rank} with $q=1$ gives
40
+ \[
41
+ \tau_G(e)=\epsilon_G(e)\in\{0,1\}.
42
+ \]
43
+ We use the standard faithful-trace argument, as in
44
+ \cite[Theorem 2.1 and Remark 2.2]{BV1998}, spelling out a similarity
45
+ to a projection. Embed $\C G$ by left convolution in the group von
46
+ Neumann algebra $\mathcal N(G)$, the commutant of the right regular
47
+ representation on $\ell^2(G)$. Its canonical normalized trace is
48
+ \[
49
+ \tau_G(T)=\langle T\delta_1,\delta_1\rangle .
50
+ \]
51
+ Its faithfulness can be seen directly: if
52
+ $T\geq0$ and $\tau_G(T)=0$, then $T^{1/2}\delta_1=0$. Since $T^{1/2}$
53
+ commutes with right translations and their translates of $\delta_1$
54
+ span a dense subspace, $T^{1/2}=0$, hence $T=0$.
55
+
56
+ Set
57
+ \[
58
+ a=e^*e+(1-e)^*(1-e).
59
+ \]
60
+ For every $\xi\in\ell^2(G)$,
61
+ \[
62
+ \langle a\xi,\xi\rangle
63
+ =\|e\xi\|^2+\|(1-e)\xi\|^2
64
+ \geq \tfrac12\|\xi\|^2.
65
+ \]
66
+ Thus $a$ is positive and invertible in $\mathcal N(G)$, and a direct
67
+ multiplication gives $ae=e^*a$. With $s=a^{1/2}$, the element
68
+ $p=ses^{-1}$ satisfies $p^2=p$ and
69
+ $p^*=s^{-1}e^*s=ses^{-1}=p$. Hence $p$ is a projection, and
70
+ traciality gives $\tau_G(p)=\tau_G(e)$. If this value is zero,
71
+ faithfulness applied to $p=p^*p$ gives $p=0$. If it is one,
72
+ faithfulness applied to $1-p$ gives $p=1$. Similarity then gives
73
+ $e=0$ or $e=1$.
74
+
75
+ Now let $R$ be any commutative unital domain of characteristic zero
76
+ and write an idempotent $f\in RG$ as
77
+ $f=\sum_{g\in S}r_g g$ with $S$ finite. Put
78
+ \[
79
+ R_0=\Z[r_g:g\in S]\subseteq R,\qquad F=\operatorname{Frac}(R_0).
80
+ \]
81
+ The field $F$ is finitely generated over $\mathbb Q$, and therefore
82
+ embeds in $\C$. Indeed, send a finite transcendence basis of
83
+ $F/\mathbb Q$ to an algebraically independent tuple of complex
84
+ numbers; the resulting embedding of the rational function field
85
+ extends across the finite algebraic extension $F$ because $\C$ is
86
+ algebraically closed. The coefficientwise maps
87
+ $R_0G\hookrightarrow RG$ and $R_0G\hookrightarrow\C G$ are injective.
88
+ Thus $f^2=f$ already holds in $R_0G$, and its image in $\C G$ is an
89
+ idempotent. The complex case makes that image $0$ or $1$, and
90
+ injectivity gives the same conclusion for $f$. Only the finitely
91
+ generated coefficient field $F$ was embedded; no embedding of all
92
+ of $R$ into $\C$ is required.
93
+ \end{proof}
94
+
95
+ \begin{remark}[Algebraic and completed trace ranges]
96
+ Continue to assume that $G$ is torsion-free. Let
97
+ $j:\C G\hookrightarrow C_r^*(G)$ be the inclusion into the reduced
98
+ group $C^*$-algebra, and let
99
+ \[
100
+ j_*:K_0(\C G)\longrightarrow K_0^{\mathrm{top}}(C_r^*(G))
101
+ \]
102
+ be the comparison map to topological $K$-theory. Write
103
+ $\tau_*^{\mathrm{top}}:K_0^{\mathrm{top}}(C_r^*(G))\to\R$ for the
104
+ canonical trace pairing. It agrees with $\tau_{G,*}$ on this image:
105
+ the same positive similarity used above, applied in a matrix algebra
106
+ over $C_r^*(G)$, produces a projection representing the image of a
107
+ matrix idempotent, and traciality preserves its trace. Consequently
108
+ \[
109
+ \tau_*^{\mathrm{top}}\!\left(j_*K_0(\C G)\right)=\Z.
110
+ \]
111
+ This is the integer range on the algebraic image, not a statement
112
+ about every class of $K_0^{\mathrm{top}}(C_r^*(G))$. In particular,
113
+ the argument does not presume that the algebraic augmentation extends
114
+ to the reduced completion. The stronger completed idempotent question
115
+ is the Kadison--Kaplansky conjecture; see \cite[Section 1]{OW2023}.
116
+
117
+ The coefficient reduction above uses characteristic zero. An idempotent
118
+ $e\notin\{0,1\}$ would give nonzero zero divisors through $e(1-e)=0$,
119
+ so the zero-divisor conjecture would imply the idempotent conjecture.
120
+ The reverse implication is not established here.
121
+ \end{remark}
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [The Blockwise Alperin Weight Conjecture](paper.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** September 23, 2026
6
+
7
+ ## Citation
8
+
9
+ ```bibtex
10
+ @misc{OAI:The-Blockwise-Alperin-Weight-Conjecture-September-23-2026,
11
+ author = {{OpenAI}},
12
+ title = {{The Blockwise Alperin Weight Conjecture}},
13
+ howpublished = {OpenAI Math Release preprint
14
+ \href{https://github.com/openai/math/blob/main/preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/paper.pdf}{OAI:The-Blockwise-Alperin-Weight-Conjecture-September-23-2026}},
15
+ year = {2026}
16
+ }
17
+ ```
18
+
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/figures/field-tower.tex ADDED
@@ -0,0 +1,40 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \begin{figure}[!ht]
2
+ \centering
3
+ \begin{tikzpicture}[
4
+ every node/.style={font=\small},
5
+ field/.style={inner sep=4pt},
6
+ inclusion/.style={-{Stealth[length=4pt]},semithick}
7
+ ]
8
+ \begin{scope}[xshift=-3.45cm]
9
+ \node[font=\small\bfseries] at (0,4.65) {Characteristic zero};
10
+ \node[field] (kb) at (0,0) {$K_b$};
11
+ \node[field] (ks) at (-1.45,1.35) {$K_s$};
12
+ \node[field] (kbp) at (1.45,1.35) {$K_b'$};
13
+ \node[field] (l) at (-1.45,2.8) {$L$};
14
+ \node[field] (lp) at (0,4) {$L'=LK_b'$};
15
+ \draw[inclusion] (kb)--(ks);
16
+ \draw[inclusion] (kb)--(kbp);
17
+ \node[font=\footnotesize,align=left] at (1.85,.35)
18
+ {unramified\\degree $n$};
19
+ \draw[inclusion] (ks)--(l);
20
+ \draw[inclusion] (l)--(lp);
21
+ \draw[inclusion] (kbp)--(lp);
22
+ \end{scope}
23
+ \begin{scope}[xshift=3.45cm]
24
+ \node[font=\small\bfseries] at (0,4.65) {Residue fields};
25
+ \node[field] (f0) at (0,0) {$F_0$};
26
+ \node[field] (fp) at (1.45,1.35) {$F'$};
27
+ \node[field] (f) at (-1.45,2.8) {$F$};
28
+ \node[field] (s) at (0,4) {$S=FF'$};
29
+ \draw[inclusion] (f0)--(fp);
30
+ \draw[inclusion] (f0)--(f);
31
+ \draw[inclusion] (f)--(s);
32
+ \draw[inclusion] (fp)--(s);
33
+ \end{scope}
34
+ \node[font=\footnotesize,align=center] at (0,-.85)
35
+ {$\operatorname{res}(K_b)=\operatorname{res}(K_s)=F_0,
36
+ \qquad [F:F_0]=[L:K_s],\qquad [L:K_s]_p<p^h.$};
37
+ \end{tikzpicture}
38
+ \caption{The auxiliary fields in a descent arising from a small Sylow orbit. Arrows denote field inclusions. The right-hand diagram records the residues of the left-hand fields; in particular $K_b$ and $K_s$ have the same residue. The field $K_b'$ splits the marked sections, and its residue $F'$ splits their reductions. The cyclic extension $K_b'/K_b$ reduces to $F'/F_0$, and the Galois actions of $L'/L$ and $S/F$ induce the same permutations of the marked points.}
39
+ \label{fig:field-tower}
40
+ \end{figure}
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/figures/proof-interfaces.tex ADDED
@@ -0,0 +1,54 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \begin{figure}[!ht]
2
+ \centering
3
+ \begin{tikzpicture}[
4
+ every node/.style={font=\small,align=center},
5
+ stage/.style={draw=black!55,rounded corners=2pt,inner sep=7pt},
6
+ flow/.style={-{Stealth[length=5pt]},semithick}
7
+ ]
8
+ \node[stage,text width=12cm] (twist)
9
+ {Marked genus-one curve: large divisor index\\
10
+ and independent absolute field differentials\\
11
+ \Cref{sec:twist}};
12
+ \coordinate (branch-top) at ($(twist.south)+(0,-9mm)$);
13
+ \coordinate (branch-split) at ($(twist.south)+(0,-4mm)$);
14
+ \node[stage,text width=5.5cm,anchor=north] (genus)
15
+ at ($(branch-top)+(-3.2cm,0)$)
16
+ {Differential estimate and divisor-degree divisibility\\Sharp inseparable genus bound
17
+ (\Cref{sec:differentials})};
18
+ \node[stage,text width=5.5cm,anchor=north] (lift)
19
+ at ($(branch-top)+(3.2cm,0)$)
20
+ {Valued lift and marked-cover descent\\Small orbit gives an extension
21
+ with small $p$-part of its degree
22
+ (\Cref{sec:valuations})};
23
+ \node[fit=(genus)(lift),inner sep=0pt,outer sep=0pt] (branches) {};
24
+ \node[stage,text width=12cm,below=10mm of branches] (specialization)
25
+ {Section comparison, finite presentation, and connectedness\\
26
+ No such marked $J$-cover over $L$ with $[L:K_s]_p<p^h$\\
27
+ when $O_p(J)=1$
28
+ (\Cref{sec:specialization})};
29
+ \node[stage,text width=12cm,below=7mm of specialization] (count)
30
+ {Every Sylow orbit has size divisible by $p^h$\\
31
+ Uniform tuple divisibility (\Cref{thm:tuple-divisibility})};
32
+ \node[stage,text width=12cm,below=7mm of count] (blocks)
33
+ {Chain inversion and central trace limits (\Cref{sec:group})\\
34
+ $l(B)=|W_p(B)|$};
35
+ \draw[flow] (twist.south) -- (branch-split) -| (genus.north);
36
+ \draw[flow] (twist.south) -- (branch-split) -| (lift.north);
37
+ \draw[flow] (genus.south) -- (genus.south |- specialization.north);
38
+ \draw[flow] (lift.south) -- (lift.south |- specialization.north);
39
+ \draw[flow] (specialization.south) -- (count.north);
40
+ \draw[flow] (count.south) -- (blocks.north);
41
+ \end{tikzpicture}
42
+ \caption{Mathematical dependencies, not reading order. The covers are geometrically
43
+ connected $J$-Galois covers, with specified $J$-action over their field of
44
+ definition, branched only at the marked points and with inertia order
45
+ divisible by $p$ at every marked point. The two branches provide, respectively, the
46
+ genus estimate and the arithmetic realization of a hypothetical small
47
+ Sylow orbit. For sufficiently large $s$, their combination rules out such a cover over a field whose
48
+ degree has small $p$-part; the geometric cover degree is fixed at $|J|$.
49
+ The resulting uniform
50
+ divisibility supplies the counting hypothesis of the block-algebra
51
+ reduction, which is proved before the geometric construction and applied
52
+ at the end. No weight-counting theorem is used to construct the curves.}
53
+ \label{fig:proof-interfaces}
54
+ \end{figure}
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/paper.tex ADDED
@@ -0,0 +1,103 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
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+ \newcommand{\DoNotLoadEpstopdf}{}
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+ \documentclass[11pt]{article}
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+ \usepackage[T1]{fontenc}
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+ \usepackage[utf8]{inputenc}
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+ \usepackage{lmodern}
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+ \usepackage{amsmath,amssymb,amsthm,mathtools}
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+ \usepackage{enumitem,booktabs,array}
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+ \usepackage{microtype}
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+ \usepackage{xcolor}
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+ \usepackage{etoolbox}
14
+ \usepackage{tikz}
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+ \usetikzlibrary{arrows.meta,positioning,calc,fit}
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+ \usepackage[pdftex,unicode,colorlinks=true,linkcolor=blue!45!black,citecolor=green!35!black,urlcolor=blue!55!black]{hyperref}
17
+ \usepackage[nameinlink,capitalise,noabbrev]{cleveref}
18
+ \makeatletter
19
+ \def\paper@thmrefstepcounter[#1]#2{%
20
+ \let\paper@saved@refstepcounter\cref@old@refstepcounter
21
+ \let\cref@old@refstepcounter\Hy@theorem@refstepcounter
22
+ \refstepcounter[#1]{#2}%
23
+ \let\cref@old@refstepcounter\paper@saved@refstepcounter
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+ }
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+ \AddToHook{begindocument/end}{%
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+ \patchcmd\cref@thmnoarg{\refstepcounter}{\Hy@theorem@refstepcounter}{}%
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+ {\PackageError{paper}{Failed to patch theorem anchors}%
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+ {Check the hyperref and cleveref compatibility patch.}}%
29
+ \patchcmd\cref@thmoptarg{\refstepcounter}{\paper@thmrefstepcounter}{}%
30
+ {\PackageError{paper}{Failed to patch named theorem anchors}%
31
+ {Check the hyperref and cleveref compatibility patch.}}%
32
+ }
33
+ \makeatother
34
+ \hypersetup{pdftitle={The Blockwise Alperin Weight Conjecture},pdfauthor={OpenAI},pdfsubject={Modular representation theory, curve covers, and inseparable genus bounds}}
35
+ \numberwithin{equation}{section}
36
+ \newtheorem{theorem}{Theorem}[section]
37
+ \newtheorem{lemma}[theorem]{Lemma}
38
+ \newtheorem{proposition}[theorem]{Proposition}
39
+ \newtheorem{corollary}[theorem]{Corollary}
40
+ \theoremstyle{definition}
41
+ \newtheorem{definition}[theorem]{Definition}
42
+ \newtheorem{notation}[theorem]{Notation}
43
+ \newtheorem{foundation}{Foundation}
44
+ \theoremstyle{remark}
45
+ \newtheorem{remark}[theorem]{Remark}
46
+ \AddToHook{env/theorem/begin}{\crefalias{theorem}{theorem}}
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+ \AddToHook{env/lemma/begin}{\crefalias{theorem}{lemma}}
48
+ \AddToHook{env/proposition/begin}{\crefalias{theorem}{proposition}}
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+ \AddToHook{env/corollary/begin}{\crefalias{theorem}{corollary}}
50
+ \AddToHook{env/definition/begin}{\crefalias{theorem}{definition}}
51
+ \AddToHook{env/notation/begin}{\crefalias{theorem}{notation}}
52
+ \AddToHook{env/remark/begin}{\crefalias{theorem}{remark}}
53
+ \crefname{foundation}{Foundation}{Foundations}
54
+ \Crefname{foundation}{Foundation}{Foundations}
55
+ \DeclareMathOperator{\Irr}{Irr}
56
+ \DeclareMathOperator{\IBr}{IBr}
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+ \DeclareMathOperator{\Br}{Br}
58
+ \DeclareMathOperator{\Gal}{Gal}
59
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60
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61
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62
+ \DeclareMathOperator{\Aut}{Aut}
63
+ \DeclareMathOperator{\Hom}{Hom}
64
+ \DeclareMathOperator{\Tr}{Tr}
65
+ \DeclareMathOperator{\im}{im}
66
+ \DeclareMathOperator{\rank}{rank}
67
+ \DeclareMathOperator{\rad}{rad}
68
+ \DeclareMathOperator{\coker}{coker}
69
+ \DeclareMathOperator{\Frac}{Frac}
70
+ \DeclareMathOperator{\ord}{ord}
71
+ \newcommand{\cO}{\mathcal O}
72
+ \newcommand{\Frob}{\operatorname{Frob}}
73
+ \setlist{itemsep=3pt,topsep=5pt}
74
+ \setlength{\emergencystretch}{1.5em}
75
+ \title{The Blockwise Alperin Weight Conjecture}
76
+ \author{OpenAI}
77
+ \date{September 23, 2026}
78
+
79
+ \begin{document}
80
+ \maketitle
81
+ \begin{abstract}
82
+ We prove the numerical blockwise Alperin weight conjecture for every
83
+ finite group and every prime $p$. For each $p$-block $B$, the number of
84
+ irreducible Brauer characters in $B$ equals the number of conjugacy
85
+ classes of $B$-weights.
86
+ \end{abstract}
87
+ {\fontsize{9}{10}\selectfont
88
+ \tableofcontents
89
+ }
90
+ \clearpage
91
+
92
+ \input{sections/intro}
93
+ \input{sections/foundations}
94
+ \input{sections/group}
95
+ \input{sections/twist}
96
+ \input{sections/differentials}
97
+ \input{sections/valuations}
98
+ \input{sections/specialization}
99
+ \input{sections/consequences}
100
+
101
+ \bibliographystyle{amsplain}
102
+ \bibliography{references}
103
+ \end{document}
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/references.bib ADDED
@@ -0,0 +1,448 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
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+ author = {Boltje, Robert and Bouc, Serge and Y{\i}lmaz, Deniz},
427
+ title = {\href{https://doi.org/10.1007/s00209-026-03999-5}{On {Alperin}'s conjecture and functorial equivalence of blocks}},
428
+ journal = {Mathematische Zeitschrift},
429
+ volume = {312},
430
+ pages = {Article~112},
431
+ year = {2026},
432
+ doi = {10.1007/s00209-026-03999-5},
433
+ url = {https://doi.org/10.1007/s00209-026-03999-5},
434
+ note = {Author's version dated February 11, 2026:
435
+ \url{https://yilmazdeniz.bilkent.edu.tr/papers/alperin-functorial.pdf}}
436
+ }
437
+
438
+ @article{Chen2024,
439
+ author = {Chen, William Y.},
440
+ title = {\href{https://doi.org/10.4007/annals.2024.199.1.5}{Nonabelian level structures, {Nielsen} equivalence, and {Markoff} triples}},
441
+ journal = {Annals of Mathematics},
442
+ volume = {199},
443
+ number = {1},
444
+ year = {2024},
445
+ pages = {301--443},
446
+ doi = {10.4007/annals.2024.199.1.5},
447
+ url = {https://doi.org/10.4007/annals.2024.199.1.5}
448
+ }
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/consequences.tex ADDED
@@ -0,0 +1,171 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Further consequences}\label{sec:consequences}
2
+
3
+ The main theorem gives both numerical information about blocks and a
4
+ functorial identity. We first prove the local--global bounds stated in
5
+ \Cref{cor:block-consequences}, then record the more detailed numerical
6
+ classification and the categorical reformulation. These are consequences
7
+ of the numerical theorem through the cited results; none is an input
8
+ to the proof above.
9
+
10
+ \subsection{Local--global and principal-block bounds}
11
+
12
+ The comparison with a defect-group normalizer is local to an individual
13
+ block. Summing it over maximal-defect blocks gives the comparison with
14
+ the Sylow normalizer, while the two principal-block bounds relate the
15
+ number of simple modules to the number of classes of $p$-elements.
16
+
17
+ We use the notation of \Cref{cor:block-consequences}; in particular,
18
+ $P\in\operatorname{Syl}_p(G)$.
19
+
20
+ \begin{proof}[Proof of \Cref{cor:block-consequences}]
21
+ The local inequality and its abelian-defect equality are Alperin's Consequences~1--2
22
+ \cite{Alperin1987}, as restated in \cite[Section~3, p.~334]{HST2024};
23
+ their numerical weight-conjecture hypotheses follow from \Cref{thm:main}.
24
+ Put $N=N_G(P)$. Since $P$ is a normal Sylow $p$-subgroup of $N$,
25
+ it is a defect group of every block of $N$.
26
+ Brauer's first main theorem therefore matches all $p$-blocks of $N$
27
+ with the maximal-defect $p$-blocks of $G$; this indexing is also used in
28
+ \cite[proof of Lemma~2.14]{FMR2025}. Writing these two block sets as
29
+ $\operatorname{Bl}_p(N)$ and $\operatorname{Bl}_{p,\max}(G)$, respectively,
30
+ the local inequality gives
31
+ \[
32
+ |\IBr_p(G)|
33
+ \geq\sum_{B'\in\operatorname{Bl}_{p,\max}(G)}l(B')
34
+ \geq\sum_{b'\in\operatorname{Bl}_p(N)}l(b')
35
+ =|\IBr_p(N)|.
36
+ \]
37
+ Finally, \Cref{thm:main} supplies the only conjectural input in
38
+ Hung--Sambale--Tiep's Propositions~3.1--3.2 \cite{HST2024}, which give
39
+ the two principal-block bounds under their respective hypotheses.
40
+ \end{proof}
41
+
42
+ \subsection{Character counts and defect data}
43
+
44
+ The next consequence treats blocks whose ordinary-character count
45
+ exceeds their Brauer-character count by one. Besides giving bounds,
46
+ it specifies all possible pairs
47
+ of defect-group order and Brauer-character count, and asserts that
48
+ every listed pair is attained.
49
+
50
+ \begin{corollary}[Character-count and defect data]\label{cor:character-data}
51
+ Let $B$ be a $p$-block of a finite group with defect group $D$ of order
52
+ $p^d$, and write $k(B)=|\Irr(B)|$. If $k(B)-l(B)=1$, then the possible
53
+ numerical data $(p^d,l(B))$ are exactly the following:
54
+ \begin{enumerate}[label=\textup{(\roman*)}]
55
+ \item There are positive integers $n,m$ such that $d=nm$, every prime divisor of $n$
56
+ divides $p^m-1$, and $4\mid n$ implies $4\mid p^m-1$, with
57
+ \[
58
+ l(B)=\sum_{e\mid n}\frac{p^{em}-1}{ne}J_2(n/e),\qquad
59
+ J_2(t)=t^2\prod_{\substack{q\mid t\\q\text{ prime}}}(1-q^{-2}).
60
+ \]
61
+ \item The exceptional pairs are
62
+ \[
63
+ \begin{aligned}
64
+ (p^d,l(B))\in\{&(5^2,7),(7^2,8),(11^2,9),(11^2,35),\\
65
+ &(23^2,88),(29^2,63),(59^2,261)\}.
66
+ \end{aligned}
67
+ \]
68
+ \end{enumerate}
69
+ All listed data occur, and in every case $k(B)=l(B)+1$.
70
+ \end{corollary}
71
+
72
+ \begin{proof}
73
+ Hung, Sambale, and Tiep proved this numerical classification assuming
74
+ the numerical weight conjecture for $B$ \cite[Theorem~3.3]{HST2024}.
75
+ \Cref{thm:main} supplies that hypothesis. Their examples establishing
76
+ that every listed value occurs were already unconditional.
77
+ \end{proof}
78
+
79
+ This classifies only character-count and defect numerical data, not blocks
80
+ up to isomorphism, Morita equivalence, or derived equivalence.
81
+
82
+ \subsection{Functorial formulation}
83
+
84
+ The following formulation expresses the numerical theorem as an identity
85
+ of classes of functors. Its alternating sum runs over all strict chains;
86
+ it is not the normal-chain transform used earlier to prove the theorem.
87
+
88
+ The numerical theorem gives the functorial formulation of
89
+ Boltje, Bouc, and Y\i lmaz \cite[Conjecture~3.3]{BBY2026}.
90
+ Let $k$ and $F$ be algebraically closed fields of characteristics $p$ and
91
+ zero, respectively. We recall the objects used in this optional
92
+ formulation. A finite-dimensional $(kH,kG)$-bimodule is viewed as a
93
+ $k[H\times G]$-module by $(h,g)m=hmg^{-1}$. It is a
94
+ $p$-permutation module if its restriction to a Sylow $p$-subgroup
95
+ has a basis permuted by that subgroup. Such a $p$-permutation bimodule
96
+ is diagonal if it is also
97
+ projective as a left $kH$-module and as a right $kG$-module.
98
+ The notation $T^\Delta(H,G)$ denotes their split Grothendieck group,
99
+ with relations $[M\oplus N]=[M]+[N]$.
100
+
101
+ The category of group--central-idempotent pairs has objects $(H,c)$,
102
+ including $c=0$. A morphism from $(H,c)$ to $(H',c')$ is an
103
+ $F$-linear combination of diagonal $p$-permutation bimodule classes
104
+ selected by $c'$ on the left and $c$ on the right. Composition is
105
+ induced by tensor product over the intermediate group algebra.
106
+ In the notation of \cite[Section~2]{BBY2026}, the category of
107
+ $F$-linear functors from this category to $F$-vector spaces is
108
+ $\mathcal F\mathcal B\ell_{F,k}$.
109
+
110
+ This functor category is semisimple in characteristic zero
111
+ \cite[Section~2.5]{BBY2026}. By Yoneda, the endomorphism space of
112
+ the representable $FT^\Delta(-,H)$ is the finite-dimensional
113
+ $F$-space $FT^\Delta(H,H)$. Semisimplicity therefore forces the
114
+ representable to have finite length: each simple summand contributes an
115
+ independent projection. Its direct summands also have finite length.
116
+ Here $K_0(\mathcal F\mathcal B\ell_{F,k})$ denotes the Grothendieck
117
+ group of the finite-length subcategory, the free abelian group on
118
+ simple-functor classes. It is in this sense that classes record the
119
+ simple multiplicities used in \cite[Sections~2.5 and~3]{BBY2026}.
120
+
121
+ The bimodule $kHc$ acts by precomposition on the representable
122
+ functor $FT^\Delta(-,H)$. Its image is the direct summand
123
+ $FT^\Delta_{H,c}=FT^\Delta(-,H)\circ kHc$ associated to $(H,c)$,
124
+ using the equivalent group and pair descriptions in
125
+ \cite[Sections~2.3--2.4]{BBY2026}. In particular $c=0$ gives the
126
+ zero functor. Write $[[H,c]]_F$ for its class in
127
+ $K_0(\mathcal F\mathcal B\ell_{F,k})$.
128
+
129
+ Write $S_{1,1,F}$ for the simple
130
+ functor indexed by the trivial pair and its trivial $F$-module.
131
+ Its multiplicity in $FT^\Delta_{H,c}$ is $l(H,c)$: evaluation at
132
+ the trivial group gives the space spanned by indecomposable projective
133
+ $kHc$-modules \cite[proof of Theorem~3.4]{BBY2026}. Thus the
134
+ following identity records all simple-functor multiplicities, with
135
+ the simple-module count as its $S_{1,1,F}$ component.
136
+
137
+ \begin{corollary}[Functorial Alperin weight identity]\label{cor:functorial-awc}
138
+ Let $b$ be a block idempotent of $kG$, where $G$ is finite. Let
139
+ $\mathcal S_p(G)$ consist of all strict chains
140
+ $\sigma=(1=P_0<P_1<\cdots<P_n)$ of $p$-subgroups, including $(1)$.
141
+ Put
142
+ \[
143
+ |\sigma|=n,\qquad
144
+ G_\sigma=\bigcap_{i=0}^nN_G(P_i),\qquad
145
+ b_\sigma=\operatorname{Br}_{P_n}(b).
146
+ \]
147
+ Since $C_G(P_n)\leq G_\sigma$ and the Brauer image is invariant
148
+ under $G_\sigma$, the element $b_\sigma$ is a central idempotent
149
+ of $kG_\sigma$, possibly zero or a sum of blocks. Thus the pair
150
+ $(G_\sigma,b_\sigma)$ is an object of the category just described.
151
+ Then, summing over representatives of the $G$-conjugacy classes of chains,
152
+ \[
153
+ \sum_{\sigma\in[G\backslash\mathcal S_p(G)]}
154
+ (-1)^{|\sigma|}[[G_\sigma,b_\sigma]]_F
155
+ =\begin{cases}
156
+ [S_{1,1,F}],&\text{if $b$ has defect zero},\\
157
+ 0,&\text{if $b$ has positive defect}
158
+ \end{cases}
159
+ \quad\text{in }K_0(\mathcal F\mathcal B\ell_{F,k}).
160
+ \]
161
+ \end{corollary}
162
+
163
+ \begin{proof}
164
+ Boltje--Bouc--Y\i lmaz first prove that, for every group--block pair,
165
+ the alternating sum above is an integer multiple of $[S_{1,1,F}]$:
166
+ every other simple-functor multiplicity cancels
167
+ \cite[Theorem~3.5\textup{(1)}]{BBY2026}. The universal numerical
168
+ blockwise Alperin weight conjecture determines the remaining coefficient
169
+ through its chain formulation. Their Theorem~3.5\textup{(2)} therefore
170
+ gives the stated identity from \Cref{thm:main}.
171
+ \end{proof}
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/differentials.tex ADDED
@@ -0,0 +1,782 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Absolute differentials and the inseparable genus estimate}
2
+ \label{sec:differentials}
3
+
4
+ The two properties of the marked curve in \Cref{sec:twist} will now
5
+ give an exact lower bound for the arithmetic genus of its purely
6
+ inseparable covers. Throughout this section, a curve over a field $U$
7
+ means a regular integral projective scheme of dimension one over $U$.
8
+ It need not be geometrically regular or geometrically reduced. We set
9
+ \[
10
+ \chi(C)=\dim_U H^0(C,\mathcal O_C)-\dim_U H^1(C,\mathcal O_C),
11
+ \qquad \nu(C)=-2\chi(C).
12
+ \]
13
+ Divisor degrees and cohomology dimensions are always taken over the
14
+ stated ground field, and the degree of a vector bundle is the degree
15
+ of its determinant. Thus $\nu(C)$ retains any contribution from an
16
+ inseparable extension of the constant field.
17
+
18
+ Fix a finite group $J$ as in \Cref{thm:tuple-divisibility} and put
19
+ $m=|J|$. Only this order enters the following estimate, as a bound on
20
+ the cover degrees needed later.
21
+ Put $\kappa=\overline{\mathbb F}_p$. For each $s$, use the fields,
22
+ elliptic curve, and labels constructed in \Cref{prop:twist-index} for
23
+ that value of $s$. In particular,
24
+ $n=p^s$, $F'=\kappa(A_0^n)$, and $E_{F'}\simeq(A_0)_{F'}$.
25
+ Write $\mathcal B$ for the descended finite \'{e}tale divisor of labels;
26
+ over $F'$ it is the sum of the distinct rational points $t_1,\ldots,t_n$.
27
+ For $h\geq1$, $s\geq h$, and a finite extension $F/F_0$ with
28
+ $[F:F_0]_p\leq p^h$, we use two properties of the marked curve.
29
+ Every divisor degree on $E_F$ is divisible by $p^{s-h}$, by
30
+ \Cref{cor:index-base-change}. Over $S=FF'$, any set of the forms
31
+ $t_i^*\eta$ loses at most $h$ dimensions of independence, by
32
+ \Cref{lem:label-rank}, where $\eta$ is a nonzero invariant differential
33
+ on $A_0$.
34
+
35
+ \begin{theorem}[Exact purely inseparable genus estimate]
36
+ \label{thm:inseparable-genus}
37
+ Fix $h\ge1$ and take $s\ge h$ such that
38
+ \begin{equation}
39
+ p^{s-h}>m\bigl(h+\log_p m\bigr).
40
+ \label{eq:genus-rounding-threshold}
41
+ \end{equation}
42
+ Let $F/F_0$ be finite with $[F:F_0]_p\le p^h$, and let $Z$ be the
43
+ normalization of $E_F$ in a finite purely inseparable extension of its
44
+ function field of degree $d\le m$. Choose a compositum $S=FF'$.
45
+ The curve $Z_S$ is integral and regular. Let $r_i$ be the ramification
46
+ index of $Z_S\to E_S$ at the unique point over $t_i$.
47
+ With $\nu(Z)$ computed over $F$, one has
48
+ \begin{equation}
49
+ \frac{\nu(Z)}d\ge\sum_{i=1}^n\left(1-\frac1{r_i}\right).
50
+ \label{eq:inseparable-genus-bound}
51
+ \end{equation}
52
+ The bound is uniform in $F$, $Z$, and the tuple-class multiset used
53
+ later in the counting argument.
54
+ \end{theorem}
55
+
56
+ The proof has two parts. Absolute differentials give the same
57
+ inequality with an error of at most $h+\log_p d$. After multiplication
58
+ by $d$, the difference between the two sides is a difference of
59
+ divisor degrees over $F$, hence a multiple of $p^{s-h}$. The strict
60
+ threshold then forces this difference to be nonnegative. We develop
61
+ the differential identities first, together with the separable
62
+ ramification bound needed later in \Cref{sec:specialization}.
63
+
64
+ \subsection{Divisor degrees, duality, and separable ramification}
65
+
66
+ The required identities hold over more general fields than the
67
+ twisted-curve construction. Throughout this and the next subsection,
68
+ let $\kappa$ be any perfect field of characteristic $p$, let
69
+ $S/\kappa$ be finitely generated, and put
70
+ $\rho=\operatorname{trdeg}_\kappa S$. Curves and degrees in these two
71
+ subsections are over $S$.
72
+
73
+ The classical theory of inseparable genus change begins with Tate
74
+ \cite{Tate1952}; Schr\"oer \cite{Schroer2009} gives a modern account
75
+ for geometrically integral curves. Here absolute differentials retain
76
+ arithmetic genus without a geometric-reducedness hypothesis and also
77
+ measure ramification at the marked points.
78
+
79
+ \begin{lemma}[Degrees over the stated ground field]
80
+ \label{lem:curve-degrees}
81
+ For an invertible sheaf $\mathcal L$ on $C$,
82
+ \begin{equation}
83
+ \chi(C,\mathcal L)=\deg_S\mathcal L+\chi(C).
84
+ \label{eq:curve-euler-degree}
85
+ \end{equation}
86
+ A finite dominant morphism $f:C\to C'$ of such curves is finite flat. If
87
+ its function-field degree is $\delta$, then
88
+ \[
89
+ \deg_S f^*D=\delta\deg_S D
90
+ \quad\text{and}\quad
91
+ \deg_S f_*D'=\deg_S D'
92
+ \]
93
+ for divisors $D$ on $C'$ and $D'$ on $C$. These assertions, and Euler
94
+ characteristics, add over disjoint unions of regular integral curves.
95
+ After a finite separable extension $S_1/S$, divisor and line-bundle degrees
96
+ and coherent Euler characteristics have the same numerical values over
97
+ $S_1$ as before extension over $S$.
98
+ \end{lemma}
99
+
100
+ \begin{proof}
101
+ For a closed point $x$ put $\deg_S(x)=[\kappa(x):S]$. For any divisor $D$
102
+ the quotient in
103
+ \[
104
+ 0\longrightarrow\mathcal O_C(D)
105
+ \longrightarrow\mathcal O_C(D+x)
106
+ \longrightarrow\mathcal Q_x\longrightarrow0
107
+ \]
108
+ has length one over the DVR $\mathcal O_{C,x}$, so its dimension over $S$
109
+ is $[\kappa(x):S]$. Finite-support sheaves have no higher cohomology.
110
+ Adding and subtracting closed points proves
111
+ $\chi(\mathcal O_C(D))=\chi(C)+\deg_S D$. A rational trivialization of
112
+ $\mathcal L$ identifies it with $\mathcal O_C(D)$ for a divisor $D$, giving
113
+ \eqref{eq:curve-euler-degree}. Applied to a principal divisor, the same
114
+ formula gives degree zero, so this degree depends only on $\mathcal L$.
115
+
116
+ Locally on $C'$, the finite module $f_*\mathcal O_C$ is torsion-free over
117
+ a DVR and therefore free, of generic rank $\delta$.
118
+ For a closed point $x\in C'$ and a uniformizer $t$ there, reduction of
119
+ this free module modulo $t$ gives
120
+ \begin{equation}
121
+ \sum_{y\mapsto x}e_y[\kappa(y):\kappa(x)]=\delta,
122
+ \label{eq:local-degree-formula}
123
+ \end{equation}
124
+ where $e_y$ is the valuation of $t$ in $\mathcal O_{C,y}$.
125
+ Indeed the summand at $y$ has a filtration of length $e_y$ with
126
+ successive quotients $\kappa(y)$. Multiplication by
127
+ $[\kappa(x):S]$ proves the pullback degree formula. The pushforward
128
+ formula follows from
129
+ $f_*y=[\kappa(y):\kappa(x)]x$ and the tower formula for residue degrees.
130
+
131
+ Finite separable scalar extension preserves regularity, and a regular
132
+ curve after such extension is a disjoint union of its integral
133
+ components. Flat base change for coherent cohomology
134
+ in \Cref{foundation:cohomology} gives
135
+ \[
136
+ H^i(C_{S_1},\mathcal G_{S_1})
137
+ =H^i(C,\mathcal G)\otimes_S S_1.
138
+ \]
139
+ Thus the dimensions over the respective fields, and hence Euler
140
+ characteristics, agree. Applying
141
+ \eqref{eq:curve-euler-degree} proves the assertion for line bundles and
142
+ their Cartier divisors. In particular it also applies to a reduced
143
+ finite divisor: separable scalar extension preserves its reducedness.
144
+ \end{proof}
145
+
146
+ \begin{proposition}[The absolute determinant computes arithmetic genus]
147
+ \label{prop:absolute-genus}
148
+ The absolute cotangent sheaf $\Omega_{C/\kappa}$ is locally free of rank
149
+ $\rho+1$, and
150
+ \begin{equation}
151
+ \deg_S\det\Omega_{C/\kappa}=\nu(C).
152
+ \label{eq:absolute-determinant-genus}
153
+ \end{equation}
154
+ \end{proposition}
155
+
156
+ \begin{proof}
157
+ An affine coordinate ring of $C$ is a localization of a finitely
158
+ generated integral $\kappa$-algebra: choose a finitely generated domain
159
+ with fraction field $S$, clear the finitely many coefficients in a
160
+ presentation over $S$, and take the contraction of the defining prime
161
+ ideal before localizing. Its local rings are consequently essentially
162
+ of finite type over $\kappa$. The regularity criterion over a perfect
163
+ field in \Cref{foundation:regularity} says that these regular local rings
164
+ are local rings at smooth points of the corresponding
165
+ $\kappa$-variety. Their absolute differentials are free of rank
166
+ \[
167
+ \operatorname{trdeg}_\kappa\kappa(C)=\rho+1.
168
+ \]
169
+ The sheaf is coherent: the relative differentials over $S$ are coherent,
170
+ and $\Omega_{S/\kappa}$ is finite-dimensional, so the cotangent sequence
171
+ gives a finite presentation locally. This proves the asserted local
172
+ freeness without making a smoothness assumption over $S$.
173
+
174
+ Choose a projective embedding $i:C\hookrightarrow\mathbb P^b_S$ and let
175
+ $\mathcal I$ be its ideal sheaf. This is a regular immersion of
176
+ codimension $b-1$. Here is a local verification. Let $R$ be an ambient
177
+ regular local ring, $I$ the local ideal, and $R/I$ the regular local ring
178
+ of $C$. Their dimensions differ by $b-1$, by the dimension formula at
179
+ the common residue field. Since both are regular, the kernel of
180
+ \[
181
+ \mathfrak m_R/\mathfrak m_R^2
182
+ \longrightarrow
183
+ \mathfrak m_{R/I}/\mathfrak m_{R/I}^2
184
+ \]
185
+ has dimension $b-1$. Choose $b-1$ elements of $I$ lifting a basis of this
186
+ kernel. They form part of a regular system of parameters of $R$ and
187
+ cut out a regular local quotient of dimension $\dim(R/I)$.
188
+ The remaining ideal defining $R/I$ in that quotient is prime and must
189
+ be zero: a nonzero prime in a finite-dimensional local domain strictly
190
+ lowers the quotient dimension. Thus the chosen elements generate $I$.
191
+ It follows that $\mathcal I/\mathcal I^2$ is locally free of rank $b-1$.
192
+
193
+ The absolute conormal sequence is in fact short exact:
194
+ \begin{equation}
195
+ 0\longrightarrow\mathcal I/\mathcal I^2
196
+ \longrightarrow i^*\Omega_{\mathbb P^b_S/\kappa}
197
+ \longrightarrow\Omega_{C/\kappa}\longrightarrow0.
198
+ \label{eq:absolute-conormal}
199
+ \end{equation}
200
+ To check the left end, the kernel of the last arrow is locally free,
201
+ since the last module is locally free. Its rank is
202
+ $(b+\rho)-(1+\rho)=b-1$. The conormal sequence surjects
203
+ $\mathcal I/\mathcal I^2$ onto this kernel. A surjection between locally
204
+ free modules of the same rank is an isomorphism, proving
205
+ \eqref{eq:absolute-conormal}.
206
+
207
+ The projective space is obtained from $\mathbb P^b_\kappa$ by extending
208
+ constants. Its absolute cotangents therefore split into relative
209
+ cotangents over $S$ and the constant bundle of $\Omega_{S/\kappa}$.
210
+ Taking determinants in \eqref{eq:absolute-conormal} gives
211
+ \[
212
+ \det\Omega_{C/\kappa}
213
+ \simeq\mathcal L_c\otimes_S\det\Omega_{S/\kappa},
214
+ \qquad
215
+ \mathcal L_c=
216
+ \mathcal O_C(-b-1)\otimes
217
+ \det(\mathcal I/\mathcal I^2)^\vee.
218
+ \]
219
+ The last tensor factor is a constant line and has degree zero.
220
+
221
+ We compute the degree of $\mathcal L_c$ using the
222
+ projective-space duality in \Cref{foundation:duality}.
223
+ A Koszul resolution for the local regular sequence defining $C$ shows
224
+ that
225
+ \[
226
+ \mathcal E xt^v_{\mathbb P^b_S}
227
+ (i_*\mathcal O_C,\mathcal O(-b-1))
228
+ =\begin{cases}
229
+ i_*\mathcal L_c,&v=b-1,\\
230
+ 0,&v\ne b-1.
231
+ \end{cases}
232
+ \]
233
+ After dualizing the Koszul resolution, its top cohomology
234
+ is the dual of the top exterior power of the free module of equations,
235
+ restricted to $C$. A change of those equations acts on this exterior
236
+ power by the determinant of their change on $\mathcal I/\mathcal I^2$.
237
+ Thus the local top cohomology modules glue to
238
+ $\det(\mathcal I/\mathcal I^2)^\vee\otimes\mathcal O_C(-b-1)$.
239
+
240
+ The local-to-global Ext spectral sequence has only this one nonzero
241
+ row. Projective-space duality consequently gives, for $r=0,1$,
242
+ \[
243
+ H^r(C,\mathcal O_C)^\vee
244
+ \simeq
245
+ \operatorname{Ext}^{b-r}_{\mathbb P^b_S}
246
+ (i_*\mathcal O_C,\mathcal O(-b-1))
247
+ \simeq H^{1-r}(C,\mathcal L_c).
248
+ \]
249
+ Hence $\chi(C,\mathcal L_c)=-\chi(C)$. Applying
250
+ \eqref{eq:curve-euler-degree} yields
251
+ $\deg_S\mathcal L_c=-2\chi(C)$, which proves
252
+ \eqref{eq:absolute-determinant-genus}.
253
+ \end{proof}
254
+
255
+ \begin{lemma}[A separable determinant bound, including the wild term]
256
+ \label{lem:separable-different}
257
+ Let $f:C\to C'$ be a finite dominant, generically separable morphism of
258
+ regular integral projective curves over $S$, of degree $\delta$.
259
+ There is an effective divisor $R_f$ on $C$ such that
260
+ \[
261
+ \nu(C)=\delta\nu(C')+\deg_S R_f.
262
+ \]
263
+ If $y\in C$ has ramification index $a_y$ over $f(y)$, then
264
+ \begin{equation}
265
+ \operatorname{ord}_y R_f\ge a_y-1+\mathbf 1_{p\mid a_y}.
266
+ \label{eq:separable-different-bound}
267
+ \end{equation}
268
+ No separability of $\kappa(y)/\kappa(f(y))$ is required.
269
+ The formula and the inequalities can be added componentwise after a
270
+ finite separable extension of $S$.
271
+ \end{lemma}
272
+
273
+ \begin{proof}
274
+ The morphism
275
+ $f^*\Omega_{C'/\kappa}\to\Omega_{C/\kappa}$ is generically an isomorphism:
276
+ at the function fields a finite separable extension has no relative
277
+ differentials, and both absolute differential spaces have dimension
278
+ $\rho+1$. Its determinant is therefore a nonzero regular morphism of
279
+ line bundles. The divisor of this morphism is effective; call it $R_f$.
280
+ Its degree is the difference of the two determinant degrees, which is
281
+ $\nu(C)-\delta\nu(C')$ by
282
+ \Cref{lem:curve-degrees,prop:absolute-genus}.
283
+
284
+ Write $x=f(y)$ and choose a uniformizer $t$ of the DVR
285
+ $B=\mathcal O_{C',x}$. Its absolute differential is primitive in
286
+ $\Omega_{B/\kappa}$, meaning that it is part of a $B$-basis. Indeed the
287
+ conormal sequence for the residue field is
288
+ \[
289
+ (t)/(t^2)\longrightarrow
290
+ \Omega_{B/\kappa}\otimes_B\kappa(x)
291
+ \longrightarrow\Omega_{\kappa(x)/\kappa}\longrightarrow0.
292
+ \]
293
+ The middle term has dimension $\rho+1$ and the right term dimension
294
+ $\rho$, since $\kappa(x)$ is finite over $S$ and
295
+ \Cref{foundation:fields} computes absolute differential dimension over
296
+ the perfect field $\kappa$. Thus the first map has nonzero
297
+ one-dimensional image, generated by $dt$. Consequently $dt$ is
298
+ nonzero modulo the maximal ideal, and it extends to a basis of the
299
+ free module $\Omega_{B/\kappa}$.
300
+
301
+ In $A=\mathcal O_{C,y}$ write $t=u\tau^{a_y}$, where $u$ is a unit and
302
+ $\tau$ a uniformizer. Absolute differentiation gives
303
+ \[
304
+ dt=\tau^{a_y}\,du+
305
+ a_yu\tau^{a_y-1}\,d\tau.
306
+ \]
307
+ All coordinates of this column of the differential matrix are
308
+ divisible by $\tau^{a_y-1}$; when $p\mid a_y$, the second term is zero,
309
+ so they are divisible by $\tau^{a_y}$. Expanding the determinant in
310
+ this column proves \eqref{eq:separable-different-bound}. Every step
311
+ uses absolute differentials over $\kappa$, so an inseparable extension
312
+ of residue fields causes no change to the argument.
313
+ \end{proof}
314
+
315
+ \subsection{The differential calculation for a height-one map}
316
+
317
+ We have established the determinant formula for arithmetic genus and
318
+ the separable ramification bound. The remaining ingredient is an
319
+ exact genus identity for a purely inseparable map of exponent one;
320
+ successive such maps will handle arbitrary purely inseparable covers.
321
+
322
+ Write $T_C=(\Omega_{C/\kappa})^\vee$ for the absolute tangent bundle.
323
+ It has rank $\rho+1$, even when the relative tangent sheaf over $S$ has
324
+ different behavior.
325
+
326
+ The calculation below is a curve-level form of the canonical-bundle
327
+ formula for a $p$-closed foliation; compare
328
+ \cite[Section~I.1, Proposition~1.1 and Equations~(1.2)--(1.3)]{Ekedahl1988}.
329
+ We prove the version needed here directly from local presentations,
330
+ using absolute differentials over the perfect constants. In this way
331
+ the kernel, the Frobenius-power cokernel, and all inseparable residue
332
+ extensions remain explicit.
333
+
334
+ \begin{lemma}[Height-one kernels and cokernels]
335
+ \label{lem:height-one}
336
+ Let $\pi:C\to C'$ be a finite dominant morphism of regular integral
337
+ projective curves over $S$ such that
338
+ $\kappa(C)^p\subseteq\kappa(C')$. Put
339
+ $q=[\kappa(C):\kappa(C')]=p^a$ and
340
+ \[
341
+ \mathcal F=\ker(T_C\longrightarrow\pi^*T_{C'}),
342
+ \qquad
343
+ \mathcal Q=\operatorname{coker}(T_C\longrightarrow\pi^*T_{C'}).
344
+ \]
345
+ Both $\mathcal F$ and $\mathcal Q$ are locally free of rank $a$, and
346
+ \begin{equation}
347
+ \det\mathcal Q\simeq(\det\mathcal F)^{\otimes p}.
348
+ \label{eq:height-one-cokernel}
349
+ \end{equation}
350
+ Consequently
351
+ \begin{equation}
352
+ \nu(C)=q\nu(C')+(p-1)\deg_S\mathcal F.
353
+ \label{eq:height-one-genus}
354
+ \end{equation}
355
+ \end{lemma}
356
+
357
+ \begin{proof}
358
+ \textit{The integral presentation.}
359
+ On an affine open of $C'$, every element of the finite upstairs
360
+ coordinate ring has its $p$th power in the downstairs ring: the power
361
+ lies in the downstairs fraction field and is integral, so normality
362
+ puts it in that ring. There is therefore a unique prime upstairs over
363
+ each downstairs prime, since membership of an element is determined
364
+ by membership of its $p$th power. At a closed point we may consequently
365
+ write $B\subset A$ for the downstairs and upstairs DVRs, with $A$ still
366
+ finite over $B$. It is finite free of rank $q$ and satisfies
367
+ $A^p\subset B$.
368
+
369
+ Let $\tau$ be an upstairs uniformizer, let $\epsilon$ be the
370
+ ramification index, and put $f=[\kappa(A):\kappa(B)]$.
371
+ The element $\tau^p\in B$ has upstairs valuation $p$; all nonzero
372
+ elements of $B$ have upstairs valuation in $\epsilon\mathbb Z$.
373
+ Thus $\epsilon\mid p$, so $\epsilon$ is $1$ or $p$.
374
+ Reduction of the rank-$q$ free module modulo a downstairs uniformizer
375
+ gives $q=\epsilon f$ by \eqref{eq:local-degree-formula}.
376
+ The residue extension has exponent at most one. Successively
377
+ adjoining a generator outside the preceding residue field gives a
378
+ degree-$p$ extension each time. Choose residue generators
379
+ $\bar b_1,\ldots,\bar b_r$ in this manner, so their monomials with
380
+ exponents in $\{0,\ldots,p-1\}$ form a $\kappa(B)$-basis of $\kappa(A)$
381
+ and $f=p^r$. Lift them to $b_1,\ldots,b_r\in A$. If $\epsilon=p$,
382
+ append $b_{r+1}=\tau$; if $\epsilon=1$, append nothing. In both cases
383
+ there are exactly $a$ generators, and $c_\ell=b_\ell^p$ belongs to $B$.
384
+
385
+ For a downstairs uniformizer $t$, the ideal $tA$ is
386
+ $\tau^\epsilon A$. Filter $A/tA$ by the powers of $\tau$ from $0$ to
387
+ $\epsilon$. Each successive quotient is $\kappa(A)$, and the lifted
388
+ residue monomials give its basis after multiplication by the
389
+ corresponding power of $\tau$. It follows that the $q$ monomials
390
+ \[
391
+ b_1^{i_1}\cdots b_a^{i_a},\qquad 0\le i_\ell<p,
392
+ \]
393
+ are a $\kappa(B)$-basis of $A/tA$.
394
+ By Nakayama they generate $A$ over $B$; since $A$ is free of rank $q$,
395
+ they are a $B$-basis. The homomorphism from the monic-relation algebra
396
+ therefore gives the actual presentation
397
+ \begin{equation}
398
+ A\simeq
399
+ B[X_1,\ldots,X_a]/(X_1^p-c_1,\ldots,X_a^p-c_a),
400
+ \qquad X_\ell\longmapsto b_\ell.
401
+ \label{eq:height-one-dvr-presentation}
402
+ \end{equation}
403
+ Both sides have the same free monomial basis over $B$, which verifies
404
+ that there are no further relations. This includes the cases of a
405
+ nontrivial inseparable residue extension and simultaneous residue
406
+ extension and ramification.
407
+
408
+ These presentations are available on open neighborhoods. Shrink an
409
+ open downstairs around the chosen point so that all the $b_\ell$ are
410
+ sections of $\pi_*\mathcal O_C$, all the $c_\ell$ are regular downstairs,
411
+ and the determinant of the displayed monomial basis is invertible.
412
+ Then \eqref{eq:height-one-dvr-presentation} holds there. Such
413
+ neighborhoods give local presentations throughout the curves.
414
+
415
+ \textit{Free kernel and free cokernel.}
416
+ Set $N=A\otimes_B\Omega_{B/\kappa}$, and let $W\subset N$ be the span
417
+ of $dc_1,\ldots,dc_a$. Differentiating the displayed presentation,
418
+ using characteristic $p$, gives
419
+ \begin{equation}
420
+ \Omega_{A/\kappa}\simeq
421
+ (N/W)\oplus\bigoplus_{\ell=1}^a A\,db_\ell.
422
+ \label{eq:height-one-differential-presentation}
423
+ \end{equation}
424
+ Both $N$ and $\Omega_{A/\kappa}$ are free of rank $\rho+1$ by
425
+ \Cref{prop:absolute-genus}. The summand $N/W$ in
426
+ \eqref{eq:height-one-differential-presentation} is therefore free,
427
+ of rank $\rho+1-a$. The sequence
428
+ $0\to W\to N\to N/W\to0$ splits, so $W$ is free of rank $a$.
429
+ Its $a$ generators $dc_\ell$ are consequently a basis.
430
+
431
+ Dualizing now shows that the tangent kernel consists of the
432
+ $\kappa$-derivations $A\to A$ killing $B$, and has free coordinates
433
+ \[
434
+ D\longmapsto(D(b_1),\ldots,D(b_a)).
435
+ \]
436
+ The tangent cokernel is $W^\vee$, with coordinates
437
+ \[
438
+ [\delta]\longmapsto
439
+ (\delta(c_1),\ldots,\delta(c_a)),
440
+ \qquad \delta\in\operatorname{Der}_\kappa(B,A).
441
+ \]
442
+ Indeed a derivation $B\to A$ extends to $A$ exactly when it kills
443
+ the $c_\ell$; when it does, the values assigned to the $b_\ell$ are
444
+ arbitrary. Thus both kernel and cokernel are locally free of rank $a$.
445
+
446
+ \textit{Gluing the determinant lines.}
447
+ On an overlap, write another system of generators as
448
+ $b'_k=P_k(b_1,\ldots,b_a)$ with coefficients in $B$, and put
449
+ \[
450
+ \mathsf J_{k\ell}=
451
+ \frac{\partial P_k}{\partial X_\ell}(b_1,\ldots,b_a).
452
+ \]
453
+ A derivation in the kernel kills the coefficients, so its new
454
+ coordinate vector is $\mathsf J$ times its old coordinate vector.
455
+ The matrix $\mathsf J$ is invertible since both coordinate systems are bases.
456
+ Taking $p$th powers of the generator identities gives downstairs
457
+ \[
458
+ c'_k=(b'_k)^p=P_k^{[p]}(c_1,\ldots,c_a),
459
+ \]
460
+ where $P_k^{[p]}$ means that the coefficients of $P_k$ are raised to
461
+ the $p$th power. Their absolute differentials vanish. Differentiating
462
+ this identity by a representative $\delta:B\to A$ of a cokernel class
463
+ therefore gives
464
+ \[
465
+ \delta(c'_k)=\sum_\ell \mathsf J_{k\ell}^{p}\,\delta(c_\ell).
466
+ \]
467
+ Thus the cokernel coordinate transition is the entrywise Frobenius
468
+ power $\mathsf J^{[p]}$. Coordinate transitions for determinant lines are
469
+ $\det\mathsf J$ and $\det(\mathsf J^{[p]})=(\det\mathsf J)^p$; if one uses local frames
470
+ instead, both transitions are inverted. In either convention they
471
+ give exactly \eqref{eq:height-one-cokernel}, with the exponent $+p$.
472
+
473
+ Finally the exact sequence
474
+ \[
475
+ 0\longrightarrow\mathcal F\longrightarrow T_C
476
+ \longrightarrow\pi^*T_{C'}\longrightarrow\mathcal Q
477
+ \longrightarrow0
478
+ \]
479
+ and \eqref{eq:height-one-cokernel} give
480
+ \[
481
+ \deg T_C=q\deg T_{C'}-(p-1)\deg\mathcal F.
482
+ \]
483
+ Since $\deg T_C=-\nu(C)$, this is \eqref{eq:height-one-genus}.
484
+ \end{proof}
485
+
486
+ \subsection{Proof of the exact estimate}
487
+
488
+ Return to the fields and marked curve in
489
+ \Cref{thm:inseparable-genus}, with $\kappa=\overline{\mathbb F}_p$
490
+ and $S=FF'$. The height-one identity will be applied along a
491
+ Frobenius tower from $Z_S$ to $E_S$. At each stage the label
492
+ covectors bound the degree of the tangent-map image; the resulting
493
+ weighted sum gives the bounded-error estimate before the final
494
+ index argument removes the error.
495
+
496
+ \begin{proof}[Proof of \Cref{thm:inseparable-genus}]
497
+ \textit{Normalization and the separable splitting field.}
498
+ Normalizations are finite by \Cref{foundation:normalization}, and normal
499
+ curves over fields are regular. We first record why the finite purely
500
+ inseparable maps in this argument are radicial, that is, universally
501
+ injective. If $A$ is the integral closure of a normal affine domain
502
+ $B$ in a finite purely inseparable extension, there is an exponent $v$
503
+ such that $a^{p^v}\in B$ for every $a\in A$. The power belongs to
504
+ $\operatorname{Frac}(B)$ and is integral over $B$, so it belongs to $B$
505
+ by normality. After tensoring with any $B$-algebra, the $p^v$th power
506
+ of every element still lies in the image of that algebra. Consequently
507
+ over a prime of the base there is at most one prime upstairs: membership
508
+ of an element in a prime is determined by membership of its $p^v$th
509
+ power downstairs. The residue extension is purely inseparable for
510
+ the same reason. This proves the assertion after every base change.
511
+
512
+ The extension $S/F$ is finite separable, since $F'/F_0$ is finite
513
+ Galois. Thus $Z_S$ is regular and reduced by
514
+ \Cref{foundation:regularity}. Its map to the integral curve $E_S$ is
515
+ still finite, surjective, and radicial. This map is a homeomorphism
516
+ on underlying spaces, so $Z_S$ is irreducible and hence integral.
517
+ It is the normalization of $E_S$ in its function field: it is finite
518
+ and normal with that field, and an element integral over the base is
519
+ also integral over its finite normal coordinate ring. Its degree
520
+ remains $d$ by finite flatness. By \Cref{lem:curve-degrees},
521
+ \[
522
+ \nu(Z_S)=\nu(Z),
523
+ \]
524
+ where the two Euler characteristics are computed over their stated
525
+ fields. We may therefore do the differential calculation over $S$.
526
+ If $d=1$, this curve is $E_S$, every $r_i=1$, and the theorem holds.
527
+ Assume henceforth that $d>1$.
528
+
529
+ \textit{The Frobenius tower and its recurrence.}
530
+ Let $M_e=S(E)$ and $M_z=S(Z)$, and set
531
+ \[
532
+ M_j=M_eM_z^{p^j}\quad(0\le j\le b),\qquad
533
+ M_0=M_z,\qquad M_b=M_e,
534
+ \]
535
+ where $b$ is the first index for which the last equality holds.
536
+ Let $Y_j$ be the normalization of $E_S$ in $M_j$, and write
537
+ \[
538
+ \gamma_j:Y_j\longrightarrow E_S,\qquad
539
+ d_j=[M_j:M_e],\qquad
540
+ \pi_j:Y_j\longrightarrow Y_{j+1},\qquad
541
+ q_j=d_j/d_{j+1}=p^{m_j}.
542
+ \]
543
+ In particular $Y_0=Z_S$, $d_0=d$, $Y_b=E_S$, and $d_b=1$.
544
+ The defining fields satisfy
545
+ \begin{equation}
546
+ M_{j+1}=M_eM_j^p.
547
+ \label{eq:frobenius-tower-field}
548
+ \end{equation}
549
+ Thus each $\pi_j$ has exponent at most one and
550
+ \Cref{lem:height-one} applies.
551
+
552
+ Put $T_j=(\Omega_{Y_j/\kappa})^\vee$ and
553
+ \[
554
+ \mathcal F_j=\ker(T_j\longrightarrow\pi_j^*T_{j+1}).
555
+ \]
556
+ This is also the kernel of the composite tangent map
557
+ $T_j\to\gamma_j^*T_{E_S}$. To see this, at the function field a
558
+ $\kappa$-derivation kills $M_e$ if and only if it kills
559
+ $M_eM_j^p=M_{j+1}$, since every derivation kills $p$th powers.
560
+ The two kernels are therefore equal generically. They are equal as
561
+ sheaves: a section whose image vanishes generically has zero image
562
+ everywhere in either of the locally free, hence torsion-free, targets.
563
+
564
+ The genus identity involves $\deg_S\mathcal F_j$. We will estimate
565
+ this degree through the image of the tangent map to $E_S$.
566
+ Choose a nonzero invariant differential $\eta$ on $A_0$.
567
+ The constant-curve identification of $E_S$ gives the splitting
568
+ \[
569
+ \Omega_{E_S/\kappa}
570
+ \simeq\mathcal O_{E_S}\eta
571
+ \oplus(\mathcal O_{E_S}\otimes_S\Omega_{S/\kappa}).
572
+ \]
573
+ Thus its dual is a trivial bundle of rank $n+1$. In this trivial
574
+ target we can use the marked points to impose linear vanishing
575
+ conditions on the tangent-map image.
576
+
577
+ Let $\mathcal H_j$ be the image in $\gamma_j^*T_{E_S}$, and put
578
+ $b_j^\circ=-\deg_S\mathcal H_j$.
579
+ It is a torsion-free coherent sheaf on a regular curve, hence locally
580
+ free. Its rank is $n+1-m_j$, since
581
+ $\operatorname{trdeg}_\kappa S=n$.
582
+ The exact sequence with kernel $\mathcal F_j$ and image $\mathcal H_j$,
583
+ together with \eqref{eq:height-one-genus}, gives
584
+ \[
585
+ \nu(Y_j)=q_j\nu(Y_{j+1})+(p-1)\deg_S\mathcal F_j,
586
+ \qquad
587
+ b_j^\circ=\nu(Y_j)+\deg_S\mathcal F_j.
588
+ \]
589
+ Eliminating $\deg_S\mathcal F_j$ and using $d_j=q_jd_{j+1}$ yields
590
+ \begin{equation}
591
+ \frac{\nu(Y_j)}{d_j}
592
+ =\frac1p\frac{\nu(Y_{j+1})}{d_{j+1}}
593
+ +\left(1-\frac1p\right)\frac{b_j^\circ}{d_j}.
594
+ \label{eq:genus-recurrence}
595
+ \end{equation}
596
+ The terminal term $\nu(Y_b)$ is zero because $E_S$ has genus one.
597
+ It remains to give a lower bound for
598
+ $b_j^\circ/d_j=-\deg_S\mathcal H_j/d_j$.
599
+
600
+ \textit{Vanishing at a ramified label.}
601
+ For each $j$ let $S_j$ be the set of labels at which $\gamma_j$ has
602
+ ramification index greater than one. For $i\in S_j$ write
603
+ $D_{j,i}=\gamma_j^*(t_i)$ and
604
+ \[
605
+ v_i=(1,-t_i^*\eta)\in S\oplus\Omega_{S/\kappa}.
606
+ \]
607
+ Regard $v_i$ as a constant linear functional on
608
+ $\gamma_j^*T_{E_S}$. We claim that its restriction to $\mathcal H_j$
609
+ vanishes along the entire divisor $D_{j,i}$; equivalently, its values
610
+ lie in $\mathcal O_{Y_j}(-D_{j,i})$.
611
+
612
+ Let $a$ be a local parameter defining the rational point $t_i$ on
613
+ $E_S$. Restriction of absolute differentials along $t_i$ sends
614
+ $(\lambda,\beta)$ in the displayed splitting to
615
+ $\lambda t_i^*\eta+\beta$. Its kernel is the line spanned by $v_i$.
616
+ Since $a$ restricts to zero, $da$ belongs to this kernel modulo $(a)$.
617
+ Moreover its relative component is nonzero: $t_i$ is an $S$-rational
618
+ point on a smooth curve over $S$, and $a$ generates its relative
619
+ cotangent space. Hence
620
+ \[
621
+ da\equiv\lambda_i v_i\pmod{a\Omega_{E_S/\kappa}}
622
+ \quad\text{for some }\lambda_i\in S^\times.
623
+ \]
624
+ At the unique point upstairs write $a=u\tau^r$, with $u$ a unit.
625
+ The nontrivial purely inseparable index $r$ is divisible by $p$;
626
+ therefore
627
+ \[
628
+ d(\gamma_j^*a)=\tau^r\,du=(\gamma_j^*a)\,u^{-1}du.
629
+ \]
630
+ It lies in the ideal of the \emph{full} divisor $D_{j,i}$ times
631
+ $\Omega_{Y_j/\kappa}$. Pulling back the preceding congruence and
632
+ dividing by the unit $\lambda_i$ shows that the pullback of $v_i$ lies
633
+ in that same ideal times $\Omega_{Y_j/\kappa}$.
634
+ To relate this differential to the claimed functional, denote the
635
+ tangent map by $d\gamma_j:T_j\to\gamma_j^*T_{E_S}$ and write
636
+ $\gamma_j^*v_i$ for the image of the pulled-back covector in
637
+ $\Omega_{Y_j/\kappa}$. For a local section $\theta$ of $T_j$, duality
638
+ gives
639
+ \[
640
+ v_i(d\gamma_j(\theta))=(\gamma_j^*v_i)(\theta).
641
+ \]
642
+ The divisibility just proved makes this value a section of
643
+ $\mathcal O_{Y_j}(-D_{j,i})$. Since $\mathcal H_j$ is the image of
644
+ $d\gamma_j$, the claim follows. The vanishing is along
645
+ $\gamma_j^*(t_i)$ with its full multiplicity, not just its reduced
646
+ support.
647
+
648
+ \textit{From independent vanishing conditions to a degree bound.}
649
+ By \Cref{lem:label-rank}, among the $v_i$ for $i\in S_j$ there are
650
+ $c\ge |S_j|-h$ independent covectors over $S$.
651
+
652
+ Complete the $c$ chosen covectors to a constant basis of the dual of
653
+ the target trivial tangent bundle. The full-divisor constraint gives
654
+ an injection
655
+ \begin{equation}
656
+ \mathcal H_j\hookrightarrow
657
+ \mathcal O_{Y_j}^{n+1-c}\oplus
658
+ \bigoplus_{i\ \mathrm{chosen}}\mathcal O_{Y_j}(-D_{j,i}).
659
+ \label{eq:label-image-injection}
660
+ \end{equation}
661
+ Let $R=n+1-m_j$ be the rank of $\mathcal H_j$.
662
+ The $R$th exterior power of the bundle on the right is a direct sum
663
+ of line bundles, each the tensor product of a choice of $R$ summands.
664
+ The induced
665
+ map from $\det\mathcal H_j$ is nonzero, so it has a nonzero component
666
+ in at least one of these lines. Only $n+1-c$ of the available
667
+ summands are trivial. The chosen line must therefore contain at least
668
+ $R-(n+1-c)=c-m_j$ negative divisor summands when this number is
669
+ positive, and at least zero otherwise.
670
+ Each $D_{j,i}$ has degree $d_j$ by finite flatness and rationality of
671
+ $t_i$. If the nonzero component uses $k$ negative summands, its target
672
+ line has degree $-kd_j$. A nonzero regular map from one line bundle
673
+ to another has an effective zero divisor, and consequently
674
+ \[
675
+ \deg_S\mathcal H_j\le-kd_j,
676
+ \qquad
677
+ \frac{b_j^\circ}{d_j}\ge c-m_j\ge |S_j|-h-m_j.
678
+ \]
679
+ The argument also covers rank zero, with $\det(0)=\mathcal O$.
680
+
681
+ \textit{The weighted estimate.}
682
+ Write $r_i=p^{u_i}$. Every height-one step has local index at most
683
+ $p$, as proved in \Cref{lem:height-one}. The composite
684
+ $Y_0\to Y_j$ consequently has ramification index at most $p^j$ at
685
+ this label. In particular, $u_i\leq b$. Since ramification indices
686
+ multiply, the remaining map
687
+ $Y_j\to E_S$ has index at least $p^{u_i-j}$ whenever $j<u_i$.
688
+ Hence $i\in S_j$ for every $0\le j<u_i$. Iterating
689
+ \eqref{eq:genus-recurrence} with terminal value zero gives
690
+ \[
691
+ \frac{\nu(Z)}d
692
+ =\sum_{j=0}^{b-1}
693
+ p^{-j}\left(1-\frac1p\right)\frac{b_j^\circ}{d_j}.
694
+ \]
695
+ Write $w_j=p^{-j}(1-1/p)$ for the weight of stage $j$. For each
696
+ label, the weights from those first $u_i$ stages sum to
697
+ \[
698
+ \sum_{j=0}^{u_i-1}p^{-j}\left(1-\frac1p\right)
699
+ =1-p^{-u_i}=1-\frac1{r_i}.
700
+ \]
701
+ Summing these contributions by label gives
702
+ \[
703
+ \sum_{j=0}^{b-1}w_j|S_j|
704
+ =\sum_{i=1}^n\sum_{\substack{0\leq j<b\\i\in S_j}}w_j
705
+ \geq\sum_{i=1}^n\left(1-\frac1{r_i}\right).
706
+ \]
707
+ The error terms in the degree bound contribute separately. Since
708
+ $m_j\le\log_p d$ and the sum of all the weights is $1-p^{-b}<1$,
709
+ \[
710
+ \sum_{j=0}^{b-1}w_j(h+m_j)\leq h+\log_p d.
711
+ \]
712
+ Substitute $b_j^\circ/d_j\geq |S_j|-h-m_j$ in the recurrence sum.
713
+ Subtracting the error bound from the label contribution yields
714
+ \begin{equation}
715
+ \frac{\nu(Z)}d
716
+ \ge\sum_{i=1}^n\left(1-\frac1{r_i}\right)
717
+ -\bigl(h+\log_p d\bigr).
718
+ \label{eq:genus-approximate}
719
+ \end{equation}
720
+
721
+ \textit{Divisors over $F$ and exact rounding.}
722
+ Multiplying \eqref{eq:genus-approximate} by $d$ bounds the possible
723
+ deficit by $d(h+\log_p d)$. Set $N=p^{s-h}$ and consider the difference
724
+ \[
725
+ A=\nu(Z)-d\sum_i\left(1-\frac1{r_i}\right).
726
+ \]
727
+ We will realize both terms as degrees of divisors on $Z$, each
728
+ retaining its degree under pushforward to $E_F$. The index property
729
+ \Cref{cor:index-base-change} then makes both degrees divisible by
730
+ $N$. These divisors must be defined over $F$, before the separable
731
+ extension to $S$.
732
+ By \Cref{prop:absolute-genus}, the integer $\nu(Z)$ is the degree over
733
+ $F$ of $\det\Omega_{Z/\kappa}$. A rational trivialization represents
734
+ this line bundle by a Cartier divisor on the regular integral curve
735
+ $Z$. Its pushforward to $E_F$ preserves degree over $F$, by
736
+ \Cref{lem:curve-degrees}. Thus
737
+ \[
738
+ \nu(Z)\in N\mathbb Z.
739
+ \]
740
+ This uses the absolute determinant on $Z/F$ and its Euler
741
+ characteristic over $F$, including any inseparable constant field.
742
+
743
+ Let $T$ be the reduced inverse image in $Z$ of $\mathcal B_F$.
744
+ It is an effective divisor on the regular curve $Z$.
745
+ Finite separable scalar extension preserves reducedness, so $T_S$
746
+ is the reduced inverse image of the split labels. If $z_i$ is the
747
+ unique point above the rational point $t_i$, the local degree formula
748
+ is
749
+ \[
750
+ r_i[\kappa(z_i):S]=d.
751
+ \]
752
+ It follows that
753
+ \[
754
+ \deg_F T=\deg_S T_S=\sum_i\frac d{r_i}.
755
+ \]
756
+ In particular this sum counts the full residue degrees of the reduced
757
+ points; those residue fields may be inseparable over $S$.
758
+ The divisor $\gamma^*\mathcal B_F-T$ is defined on $Z$ over $F$, where
759
+ $\gamma:Z\to E_F$, and its degree is
760
+ \[
761
+ dn-\sum_i\frac d{r_i}
762
+ =d\sum_i\left(1-\frac1{r_i}\right).
763
+ \]
764
+ Push it to $E_F$ to conclude that this integer also belongs to
765
+ $N\mathbb Z$.
766
+
767
+ Consequently $A$ is a multiple of $N$. By
768
+ \eqref{eq:genus-approximate} and $d\le m$,
769
+ \[
770
+ A\ge-d(h+\log_p d)
771
+ \ge-m(h+\log_p m)>-N.
772
+ \]
773
+ A multiple of $N$ strictly greater than $-N$ is nonnegative. This
774
+ proves \eqref{eq:inseparable-genus-bound}.
775
+ The sufficient threshold \eqref{eq:genus-rounding-threshold} contains
776
+ no datum from $F$, $Z$, or a tuple-class multiset. If a threshold
777
+ independent of the prime is desired, the stronger condition
778
+ \[
779
+ 2^{s-h}>m(h+\log_2m)
780
+ \]
781
+ suffices for every $p\ge2$. This proves the stated uniformity.
782
+ \end{proof}
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/foundations.tex ADDED
@@ -0,0 +1,167 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Classical foundations used}\label{sec:foundations}
2
+
3
+ We state the classical inputs to make the scope of the proof explicit. We also use elementary linear algebra, field and group theory, and the basic definitions and functorial formalism of schemes, sheaves, divisors, and K\"ahler differentials. The counting, index, inseparable-genus, valued-field, and specialization assertions particular to this proof are established in the later sections. In particular, no weight-counting theorem or conjectural reduction is an input.
4
+
5
+ \begin{foundation}[Finite groups]\label{foundation:groups}
6
+ For a finite group $X$, its $p$-subgroups lie in Sylow subgroups of order $|X|_p$. A nontrivial finite $p$-group has nontrivial center and an element of order $p$, and each of its maximal proper subgroups is normal. We use the orbit--stabilizer formula and the usual fixed-point and conjugation actions.
7
+ \end{foundation}
8
+
9
+ \begin{foundation}[Finite-dimensional algebras and characters]\label{foundation:algebra}
10
+ The Jacobson radical of a finite-dimensional algebra is nilpotent. Over an algebraically closed field, its semisimple quotient is a product of full matrix algebras, one for each simple module up to isomorphism. A finite-dimensional commutative algebra over an algebraically closed field is a product of local algebras with that field as residue, indexed by its primitive idempotents. Finite group algebras in characteristic zero are semisimple. Over a splitting field the simple endomorphism algebras are the scalar field, and an ordinary irreducible character satisfies
11
+ \[
12
+ \sum_{x\in X}\chi(x)\chi(x^{-1})=|X|.
13
+ \]
14
+ Idempotents lift uniquely from the residue algebra of a finite commutative algebra over a complete discrete valuation ring. Nakayama's lemma applies to finite modules over any local ring.
15
+ \end{foundation}
16
+
17
+ \begin{foundation}[Commutative algebra]\label{foundation:commalg}
18
+ A finite-type algebra over a Noetherian ring is Noetherian. Integral extensions satisfy lying over. Closed points of a variety over a field are dense and have finite residue fields over the ground field. For an integral variety, the local dimension at a point plus the transcendence degree of its residue field is the transcendence degree of the function field. A regular local ring is a normal domain; a part of a minimal system of generators of its maximal ideal is a regular sequence and its quotient is regular of the correspondingly smaller dimension. A one-dimensional Noetherian normal local domain is a discrete valuation ring, as is a Noetherian local domain with nonzero principal maximal ideal. Finite torsion-free modules over discrete valuation rings are free. Completion of a discrete valuation ring retains its residue field and uniformizer.
19
+ \end{foundation}
20
+
21
+ \begin{foundation}[Fields and absolute field differentials]\label{foundation:fields}
22
+ If a finite group $D$ acts faithfully by automorphisms on a field $M$, then $M/M^D$ is Galois of degree $|D|$. Finite separable field extensions are simple. A finite field extension has a maximal separable subextension, and the remaining extension is purely inseparable; the number of embeddings in an algebraic closure is the separable degree. Multiplicative groups of finite fields are cyclic. Algebraically closed fields are classified by their characteristic and transcendence degree. If $S$ is a finitely generated field of transcendence degree $\rho$ over a perfect field $\kappa$, then
23
+ \[
24
+ \dim_S\Omega_{S/\kappa}=\rho;
25
+ \qquad [S:S^p]=p^\rho\quad\text{in characteristic }p.
26
+ \]
27
+ \end{foundation}
28
+
29
+ \begin{foundation}[Valuations over a complete discrete base]\label{foundation:valuation}
30
+ A valuation extends to an algebraic field extension. A complete discrete valuation on a field extends uniquely to any finite field extension; its valuation ring is the integral closure of the original ring, is finite over it, and is again a complete discrete valuation ring. The fields to which we apply the latter assertion initially have characteristic zero. No corresponding finiteness assertion for an arbitrary nondiscrete valuation ring is assumed.
31
+ See \cite[Tag 00IA]{Stacks} for prolongation and
32
+ \cite[Tags 032W, 09EM and 0325]{Stacks} for the complete
33
+ discrete-base finiteness assertions.
34
+ \end{foundation}
35
+
36
+ \begin{foundation}[Descent and finite models]\label{foundation:descent}
37
+ A projective scheme with a semilinear descent datum under a finite Galois field extension descends if equipped with a compatible linearized ample line bundle. The same statement holds for a finite \emph{\'etale} faithfully flat Galois extension of rings and a relatively ample line bundle. Equivariant morphisms and invariant closed subschemes descend along with the scheme. Flatness, smoothness, finiteness, \emph{\'etaleness}, and relative ampleness in these settings are checked after the faithfully flat extension. Geometric integrality of a finite-type scheme over a field can be checked after an extension of that field. A finite diagram of projective schemes and morphisms of finite presentation over a directed union of fields is defined over a finite stage, including its maps to a base scheme already defined there and the identities among those maps. One may realize projective descent by descent of semilinear modules and graded algebras followed by $\Proj$.
38
+ For the projective and module descent assertions, see \cite[Tags 0CCJ, 0CDR and 0D1V]{Stacks}.
39
+ The five locality assertions are respectively
40
+ \cite[Tags 02L2, 02VL, 02LA, 02VN and 0D3C]{Stacks}; geometric
41
+ integrality is covered by \cite[Tags 038K, 0384 and 054P]{Stacks}.
42
+ The finite-stage assertion follows from \cite[Tags 01ZM and 01ZP]{Stacks},
43
+ including chosen projective embeddings among the finite data.
44
+ \end{foundation}
45
+
46
+ \begin{foundation}[Normalization]\label{foundation:normalization}
47
+ The normalization of an integral variety over a field in a finite extension of its function field is finite. The normalization of a finite-type $\mathbb Z$-domain in its fraction field is finite. In the integral closure of a normal domain in a finite Galois extension of its fraction field, the Galois group acts transitively on the primes above any fixed prime of the base.
48
+ The normalization finiteness assertions follow from the Nagata property in \cite[Tag 0335]{Stacks}.
49
+ \end{foundation}
50
+
51
+ \begin{foundation}[Regularity, smoothness, and properness]\label{foundation:regularity}
52
+ Finite separable scalar extension preserves regularity and reducedness. Smooth varieties over a field are regular. A regular local ring essentially of finite type over a perfect field $\kappa$ is smooth at the corresponding point of a finite-type $\kappa$-model; its module of absolute differentials is free of rank the transcendence degree of the function field over $\kappa$. We use the valuative criterion for properness, including the unique extension of maps from fraction fields of valuation rings, and that proper maps are closed.
53
+ For regularity and smoothness over a perfect field, see \cite[Tags 00TV and 0B8X]{Stacks}.
54
+ \end{foundation}
55
+
56
+ \begin{foundation}[Proper cohomology and ample section rings]\label{foundation:cohomology}
57
+ Over a Noetherian base, the higher direct images of coherent sheaves under a proper morphism are coherent. Over an affine base their cohomology commutes with flat affine base change. For a projective scheme over an affine Noetherian base and a relatively ample line bundle, sufficiently high powers give projective embeddings, and sufficiently high twists annihilate higher coherent cohomology. The ample section ring is finitely generated and its $\Proj$ recovers the scheme. Finite pullback preserves ampleness; tensor products of relatively ample line bundles are relatively ample, and a line bundle is relatively ample if a positive power is. Formation of $\Proj$ commutes with base change. On a projective curve over a field, coherent cohomology vanishes in degrees greater than one, and for sheaves of finite support in degrees greater than zero. Global functions on a geometrically integral projective variety over a field equal the ground field.
58
+ For proper coherence, flat cohomology base change, and ample twists, respectively, see \cite[Tags 02O5, 02KH and 0B5T]{Stacks}.
59
+ For Proj recovery and the ampleness rules, see
60
+ \cite[Tags 0EKI, 0892, 0890 and 02NN]{Stacks}.
61
+ \end{foundation}
62
+
63
+ \begin{foundation}[Differentials, adjunction, and duality]\label{foundation:duality}
64
+ We use the transitivity sequence
65
+ \[
66
+ \Omega_{V/U}\otimes_VW\longrightarrow\Omega_{W/U}
67
+ \longrightarrow\Omega_{W/V}\longrightarrow0
68
+ \]
69
+ and the conormal sequence for a closed immersion. Let $S$ be a field. On $\mathbb P^b_S$,
70
+ $\det\Omega_{\mathbb P^b_S/S}=\mathcal O(-b-1)$. For a coherent sheaf $\mathcal G$ there, Serre duality identifies
71
+ \[
72
+ H^i(\mathcal G)^\vee
73
+ \simeq\operatorname{Ext}^{b-i}
74
+ (\mathcal G,\mathcal O(-b-1)).
75
+ \]
76
+ We use the local-to-global Ext spectral sequence and the Koszul resolution of a quotient by a regular sequence. These inputs will yield the required absolute determinant-degree formula even when the curve is not smooth over $S$.
77
+ For the projective-space dualizing complex and the adjunction formalism, see \cite[Tag 0A9W and Section~48.15]{Stacks}.
78
+ The local-to-global Ext sequence is \cite[Tag 0BQP]{Stacks}.
79
+ \end{foundation}
80
+
81
+ \begin{foundation}[Elliptic curves]\label{foundation:elliptic}
82
+ A smooth Weierstrass cubic with its point at infinity is an elliptic curve. A generalized Weierstrass equation over a discrete valuation ring with unit discriminant gives a smooth elliptic scheme, polarized by three times its origin. Its relative cotangent line is trivial with invariant differential $\eta$, and multiplication by an integer $a$ pulls $\eta$ back to $a\eta$. For a positive integer $a$, multiplication by $a$ on an elliptic curve or elliptic scheme is finite locally free of degree $a^2$.
83
+ For the relative group law, see
84
+ \cite[II, Proposition~2.7]{DeligneRapoport1973}; the unit-discriminant
85
+ Weierstrass family and the invariant cotangent description are given in
86
+ \cite[Tags 072S and 047I]{Stacks}. See also
87
+ \cite[Chapter~III]{Silverman2009} for the Weierstrass formulation.
88
+ Multiplication is finite flat and surjective by
89
+ \cite[Proposition~20.7]{MilneAV2022}; over the Noetherian bases here it
90
+ is finite locally free by \cite[Tag 02KB]{Stacks}.
91
+ \end{foundation}
92
+
93
+ \begin{foundation}[Complex curves and covers]\label{foundation:complex}
94
+ Finite \'etale algebraic covers of a smooth complex algebraic curve
95
+ correspond to finite unramified topological covers of its analytification,
96
+ including morphisms. For a punctured projective curve, normalization of
97
+ the original projective curve in the resulting algebraic function field
98
+ gives the finite compact cover. Normal complex curves are smooth, and the
99
+ local punctured covering completes by a power map, so monodromy cycle
100
+ lengths give ramification indices. Topological covers are classified by
101
+ fundamental-group actions on finite fibers. The fundamental group of a
102
+ genus-one surface punctured at $n$ points has generators
103
+ $x,y,u_1,\ldots,u_n$ with the single relation
104
+ \[
105
+ [x,y]u_1\cdots u_n=1.
106
+ \]
107
+ For a finite map of smooth proper curves over an algebraically closed field of characteristic zero, Riemann--Hurwitz states
108
+ \[
109
+ 2g(C)-2=\deg(f)\bigl(2g(C')-2\bigr)
110
+ +\sum_{P\in C}(e_P-1).
111
+ \]
112
+ For the algebraic/topological cover correspondence, see \cite[Theorem~3.4]{MilneLEC2008}; for Riemann--Hurwitz, see \cite[Section~53.12, Tag 0C1B]{Stacks}.
113
+ \end{foundation}
114
+
115
+ \begin{foundation}[Noetherian connectedness]\label{foundation:connectedness}
116
+ A proper morphism over a locally Noetherian base whose structure-sheaf direct image is canonically the structure sheaf of the base has geometrically connected fibers. This is the connected-fiber assertion of Stein factorization. We apply it only after constructing a Noetherian normal model, not directly over the nondiscrete valuation ring.
117
+ See \cite[Tag 03H0]{Stacks}.
118
+ \end{foundation}
119
+
120
+ \subsection{Coefficient fields and scalar extension}\label{sec:coefficients}
121
+
122
+ We justify the coefficient choice in \Cref{sec:introduction} without
123
+ requiring a mixed-characteristic lift of every algebraically closed
124
+ field. Put $\kappa=\overline{\mathbb F}_p$ and choose an embedding
125
+ $\kappa\hookrightarrow k$. For any finite group $X$, the ideal
126
+ $\rad(\kappa X)\otimes_\kappa k$ is nilpotent, and the quotient of
127
+ $kX$ by this ideal is the scalar extension of the split matrix product
128
+ $\kappa X/\rad(\kappa X)$. That quotient is again a split semisimple
129
+ algebra. The ideal is therefore exactly $\rad(kX)$, and the simple
130
+ modules correspond under scalar extension.
131
+
132
+ The center also commutes with this extension: it is the kernel of the
133
+ finitely many linear maps $a\mapsto ax-xa$, $x\in X$, and field
134
+ extension preserves kernels. Each local factor of $Z(\kappa X)$ has
135
+ nilpotent radical and residue $\kappa$; after extension it still has
136
+ nilpotent radical, now with residue $k$, so remains local. Thus
137
+ primitive blocks correspond and their simple-module counts agree.
138
+ Coefficient restriction, restriction to centralizers in the Brauer
139
+ map, and the quotient maps for normal subgroups all commute with
140
+ scalar extension. The residue characters of the local central factors
141
+ extend as well. Consequently the central-character block assignment
142
+ in \eqref{eq:block-assignment} is preserved, for every subgroup and
143
+ subquotient involved in a weight. It suffices to prove the numerical
144
+ identity over $\kappa$.
145
+
146
+ To construct the coefficient ring, start with $\mathbb Z_p$, lift a
147
+ tower of finite separable extensions of its residue field $\mathbb F_p$
148
+ that exhausts $\kappa$, and complete the union. The construction at the
149
+ start of the proof of \Cref{prop:mixed-lift} shows that this gives a
150
+ complete discrete valuation ring of characteristic zero with residue
151
+ $\kappa$.
152
+ In an algebraic closure of its fraction field, choose matrix
153
+ realizations of every ordinary irreducible representation of every
154
+ subgroup of $G$. There are only finitely many such representations and
155
+ matrix entries. Adjoining their entries gives a finite field extension
156
+ that splits all those subgroups. Its valuation ring is again a complete
157
+ DVR by \Cref{foundation:valuation}; its finite residue extension is
158
+ still $\kappa$, which is algebraically closed. This gives the system
159
+ $(K,\mathcal O,\kappa)$ used in \Cref{sec:group}. Quotient
160
+ representations inflate, so the same coefficients split the required
161
+ subquotients. These coefficient fields are separate from the auxiliary
162
+ geometric fields constructed later.
163
+
164
+ The remaining sections prove the blockwise chain identity, the marked
165
+ high-index twist, the genus estimate with exact rounding, the required
166
+ valued-field assertions, and the specialization model. The foundations
167
+ above supply their classical inputs, not the desired weight equality.
preprints/The-Blockwise-Alperin-Weight-Conjecture-September-23-2026/build/sections/group.tex ADDED
@@ -0,0 +1,839 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{From block counts to generating tuples}\label{sec:group}
2
+
3
+ Fix a prime $p$. Write $O_p(X)$ for the largest normal $p$-subgroup
4
+ of a finite group $X$, and put $[x,y]=xyx^{-1}y^{-1}$. A
5
+ $p$-element includes the identity; a $p'$-element has order prime to
6
+ $p$; and a $p$-singular element has order divisible by $p$.
7
+ The geometric sections will establish the following precise counting
8
+ statement. Its uniformity is part of the assertion.
9
+
10
+ \begin{theorem}[Uniform divisibility for generating tuples]
11
+ \label{thm:tuple-divisibility}
12
+ Let $J$ be a finite group with $O_p(J)=1$. For $s\geq0$, $n=p^s$,
13
+ and a multiset
14
+ $\mathcal M$ of $n$ conjugacy classes of $p$-singular elements of $J$,
15
+ let $N_{J,s}(\mathcal M)$ be the number, modulo simultaneous
16
+ $J$-conjugation, of ordered tuples
17
+ \[
18
+ (x,y,u_1,\ldots,u_n)\in J^{n+2}
19
+ \]
20
+ satisfying
21
+ \begin{equation}\label{eq:tuple-relation}
22
+ [x,y]u_1\cdots u_n=1,\qquad
23
+ \langle x,y,u_1,\ldots,u_n\rangle=J,
24
+ \qquad \{[u_1],\ldots,[u_n]\}=\mathcal M.
25
+ \end{equation}
26
+ For every integer $h\geq1$, there is an integer $s_0=s_0(p,J,h)$
27
+ such that
28
+ \[
29
+ p^h\mid N_{J,s}(\mathcal M)
30
+ \qquad(s\geq s_0)
31
+ \]
32
+ for every such multiset $\mathcal M$.
33
+ \end{theorem}
34
+
35
+ The entries $u_i$ remain ordered: prescribing their multiset of classes
36
+ does not quotient by permutations. Empty tuple sets have count zero,
37
+ so the statement includes $J=1$ and groups of order prime to $p$.
38
+ The proof of \Cref{thm:tuple-divisibility} is completed after
39
+ \Cref{prop:no-small-cover}. This section proves that it implies the
40
+ block equality, using \Cref{foundation:groups,foundation:algebra}
41
+ and proving the required counting reductions explicitly.
42
+
43
+ \subsection{Coefficient projection and the weight transform}
44
+
45
+ For each ambient finite group $X$, choose a splitting coefficient system
46
+ $(K,\mathcal O,k)$ as in \Cref{sec:introduction,sec:coefficients}, with
47
+ $X$ in place of $G$. Hold this system fixed throughout the calculations
48
+ with $X$ and its subquotients.
49
+ This system also splits all subquotients that occur below: a subgroup of a
50
+ quotient lifts to a subgroup by taking its preimage, and a
51
+ representation of a quotient inflates to that preimage. These
52
+ observations apply after any number of subgroup and quotient steps.
53
+ Ordinary irreducibles may therefore be realized over $K$. Their
54
+ identification with complex irreducibles, when needed, follows by
55
+ first splitting the group algebra over $\overline{\mathbb Q}$ and
56
+ then extending scalars to algebraically closed characteristic-zero
57
+ fields.
58
+
59
+ For a central idempotent $E\in kX$, define
60
+ \begin{align*}
61
+ l(X,E)&=\#\{\text{simple $kX$-modules selected by $E$}\},\\
62
+ k_{\mathrm{ord}}(X,E)&=\#\{\text{ordinary irreducibles selected by the lift of $E$}\},\\
63
+ z(X,E)&=\#\{\chi\text{ selected by that lift}:\chi(1)_p=|X|_p\}.
64
+ \end{align*}
65
+ Here and throughout, modules and characters are counted up to
66
+ isomorphism. The class sums form a basis of $Z(\mathcal O X)$, and
67
+ their reductions form a basis of $Z(kX)$. Idempotent lifting over the
68
+ complete DVR thus gives a unique central idempotent lifting $E$.
69
+ Every integral central element acts on an ordinary irreducible by
70
+ a scalar in $\mathcal O$: the scalar lies in $K$ by splitting and
71
+ satisfies a monic integral equation by finiteness, and $\mathcal O$
72
+ is integrally closed. Reduction of this scalar defines a character
73
+ of $Z(kX)$. The Artinian local decomposition of that center shows
74
+ that it is precisely $\lambda_b$, where $b$ is the block containing
75
+ the ordinary irreducible.
76
+
77
+ For $H\leq X$, let $s_H$ denote coefficient restriction from
78
+ $Z(kX)$ to $Z(kH)$, or its integral analogue when appropriate.
79
+ For a $p$-subgroup $Q$, let $\operatorname{Br}_Q$ denote restriction
80
+ of coefficients from the $Q$-invariants $(kX)^Q$ to $kC_X(Q)$.
81
+
82
+ \begin{lemma}[Normalizer projection]\label{lem:normalizer-projection}
83
+ The map $\operatorname{Br}_Q:(kX)^Q\longrightarrow kC_X(Q)$ is a
84
+ unital algebra homomorphism. Suppose that
85
+ \[
86
+ Q\leq H\leq N_X(Q),\qquad C_X(Q)\leq H.
87
+ \]
88
+ Writing $\pi_Q:kH\longrightarrow k[H/Q]$ for the quotient map, one
89
+ has, for $v\in Z(kX)$,
90
+ \begin{equation}\label{eq:normalizer-projection}
91
+ \pi_Q(s_H(v))=\pi_Q(\operatorname{Br}_Q(v)),
92
+ \qquad
93
+ \lambda_b(s_H(v))=\lambda_b(\operatorname{Br}_Q(v))
94
+ \end{equation}
95
+ for every block $b$ of $H$. In particular $\lambda_b\circ s_H$ is
96
+ the central character of a unique block of $X$.
97
+ \end{lemma}
98
+
99
+ \begin{proof}
100
+ To compute the coefficient of $g\in C_X(Q)$ in a product of two
101
+ $Q$-invariant elements, let $Q$ conjugate the pairs $(a,b)$ with
102
+ $ab=g$. Coefficient products are constant on the orbits. Every
103
+ nontrivial orbit has size divisible by $p$, and the fixed pairs are
104
+ exactly those with $a,b\in C_X(Q)$. This proves multiplicativity;
105
+ the identity is preserved.
106
+
107
+ Each coset $hQ$ is stable under conjugation by $Q$, because
108
+ $h\in N_X(Q)$. Applying the same orbit cancellation to the sum
109
+ of coefficients over that coset proves the first identity in
110
+ \eqref{eq:normalizer-projection}. Also
111
+ $\operatorname{Br}_Q(v)\in Z(kH)$, since its support lies in
112
+ $C_X(Q)\leq H$ and it is invariant under $H$.
113
+
114
+ Every nonzero module for a finite $p$-group over $k$ has nonzero
115
+ invariants. For completeness, choose a central element $z$ of order
116
+ $p$; the nonzero kernel of $z-1$, whose $p$th power is zero, is a
117
+ module for the smaller group $Q/\langle z\rangle$, and induction
118
+ applies. If the module is simple for $H$, its $Q$-invariants are
119
+ $H$-stable, and hence the whole module. Thus every simple $kH$-module
120
+ factors through $H/Q$, proving the second identity. The composition
121
+ with $\operatorname{Br}_Q$ is a unital algebra character. Characters
122
+ of the finite commutative algebra $Z(kX)$ are its local residue
123
+ characters, one for each block, giving uniqueness.
124
+ \end{proof}
125
+
126
+ For $H=N_X(Q)$ put
127
+ \[
128
+ \overline E_Q
129
+ =\pi_Q(s_H(E))
130
+ =\pi_Q(\operatorname{Br}_Q(E))\in Z(k[H/Q]).
131
+ \]
132
+ This is an idempotent. Its selected defect-zero quotient characters
133
+ are exactly the weights assigned to the blocks appearing in $E$.
134
+ Indeed, the lift of $\operatorname{Br}_Q(E)$ maps to the lift of
135
+ $\overline E_Q$ by uniqueness of central idempotent lifting. Its
136
+ action on the inflation of a quotient character is therefore one
137
+ exactly when the latter is selected by $\overline E_Q$. If $b$ is
138
+ the block of this inflation, the same test is
139
+ \[
140
+ \lambda_b(\operatorname{Br}_Q(E))
141
+ =\lambda_b(s_H(E))=1.
142
+ \]
143
+ By \Cref{lem:normalizer-projection}, this says that the induced block
144
+ is one of the blocks in $E$, with the coefficient-projection
145
+ definition in \eqref{eq:block-assignment}. Once $Q$ is fixed up to $X$-conjugacy,
146
+ there is no further identification of its quotient characters:
147
+ $N_X(Q)$ acts on $N_X(Q)/Q$ by inner automorphisms.
148
+
149
+ For a conjugation-invariant function $g$ of such pairs $(X,E)$,
150
+ define
151
+ \begin{equation}\label{eq:weight-transform}
152
+ (Tg)(X,E)=
153
+ \sum_{\substack{1<Q\leq X\text{ a $p$-subgroup}\\
154
+ \text{up to }X\text{-conjugacy}}}
155
+ g\bigl(N_X(Q)/Q,\overline E_Q\bigr).
156
+ \end{equation}
157
+ Consequently the desired universal equality for block sums is
158
+ $l=(1+T)z$. The identity term includes precisely $Q=1$.
159
+ Every transition in $T$ strictly decreases the $p$-part of the group
160
+ order, so $T$ is nilpotent on each evaluated pair. Thus the formal
161
+ inverse $(1+T)^{-1}=\sum_{r\geq0}(-T)^r$ is evaluation-wise finite.
162
+
163
+ The next step makes the connection with subgroup-chain formulations of
164
+ the weight conjecture \cite{KnorrRobinson1989}. We derive the particular
165
+ normal-chain identity from this finite inverse, retaining its idempotent
166
+ and orbit data throughout.
167
+
168
+ \begin{definition}[Chains]\label{def:p-chains}
169
+ A chain in $X$ is a strictly increasing sequence of $p$-subgroups
170
+ \[
171
+ \mathcal C=(1=Q_0<Q_1<\cdots<Q_r),
172
+ \qquad |\mathcal C|=r.
173
+ \]
174
+ The length-zero chain $(1)$ is included. Set
175
+ \[
176
+ H_{\mathcal C}=\bigcap_{i=0}^rN_X(Q_i),
177
+ \qquad E_{\mathcal C}=\operatorname{Br}_{Q_r}(E).
178
+ \]
179
+ Call $\mathcal C$ \emph{normal} if every $Q_i$ is normal in $Q_r$.
180
+ \end{definition}
181
+
182
+ For every chain, normal or otherwise,
183
+ $C_X(Q_r)\leq H_{\mathcal C}\leq N_X(Q_r)$, so
184
+ $E_{\mathcal C}$ is an idempotent of $Z(kH_{\mathcal C})$.
185
+ For a normal chain one also has $Q_r\leq H_{\mathcal C}$.
186
+
187
+ \begin{lemma}[Finite chain inversion]\label{lem:chain-transform}
188
+ The identity $l=(1+T)z$ for all pairs $(X,E)$ is equivalent to
189
+ \begin{equation}\label{eq:chain-inversion}
190
+ z(X,E)=
191
+ \sum_{\substack{\mathcal C/X\\\mathcal C\ \mathrm{normal}}}
192
+ (-1)^{|\mathcal C|}l(H_{\mathcal C},E_{\mathcal C}),
193
+ \end{equation}
194
+ where $\mathcal C/X$ denotes one representative of each
195
+ $X$-conjugacy orbit.
196
+ \end{lemma}
197
+
198
+ \begin{proof}
199
+ We identify the terms of $T^r l$. After $r$ steps they correspond
200
+ to normal chains of length $r$, with group
201
+ $H_{\mathcal C}/Q_r$ and idempotent
202
+ \[
203
+ \pi_{Q_r}(s_{H_{\mathcal C}}(E))
204
+ =\pi_{Q_r}(E_{\mathcal C}).
205
+ \]
206
+ For the induction, the preimage $Q_{r+1}$ of a nontrivial
207
+ $p$-subgroup of $H_{\mathcal C}/Q_r$ is a $p$-group strictly
208
+ containing $Q_r$. It lies in $H_{\mathcal C}$ and therefore
209
+ normalizes every preceding $Q_i$. Conversely every normal one-step
210
+ extension arises in this way. Its normalizer in the quotient has
211
+ preimage
212
+ $H_{\mathcal C}\cap N_X(Q_{r+1})=H_{\mathcal C'}$.
213
+ After fixing $\mathcal C$, conjugation is by its stabilizer
214
+ $H_{\mathcal C}$, which is exactly quotient conjugation at the next
215
+ step. This proves the orbit assertion without an extra multiplicity.
216
+
217
+ To check the idempotent at the next step, write
218
+ $E=\sum_{x\in X}e_xx$ and put $H'=H_{\mathcal C'}$.
219
+ The new normalizer in $H_{\mathcal C}/Q_r$ is $H'/Q_r$.
220
+ Restriction to this normalizer retains exactly the coefficient sums
221
+ over the $Q_r$-cosets contained in $H'$. Choose a set $A$ of
222
+ representatives for the cosets of $Q_r$ in $Q_{r+1}$. For $h\in H'$,
223
+ the subsequent quotient has coefficient
224
+ \[
225
+ \sum_{a\in A}\ \sum_{q\in Q_r}e_{haq}
226
+ =\sum_{t\in Q_{r+1}}e_{ht}
227
+ \]
228
+ at $hQ_{r+1}$: the sets $aQ_r$, $a\in A$, partition $Q_{r+1}$.
229
+ These are precisely the coefficients of
230
+ $\pi_{Q_{r+1}}(s_{H'}(E))$.
231
+ By \Cref{lem:normalizer-projection}, this idempotent is
232
+ $\pi_{Q_{r+1}}(E_{\mathcal C'})$, as required.
233
+ Every simple $kH_{\mathcal C}$-module factors through
234
+ $H_{\mathcal C}/Q_r$ and has the indicated idempotent action.
235
+ Hence the contribution to $T^rl$ is the corresponding term in
236
+ \eqref{eq:chain-inversion}. The finite inverse of $1+T$ now gives
237
+ the equivalence.
238
+ \end{proof}
239
+
240
+ \subsection{Cocenters and subsections}
241
+
242
+ By \Cref{lem:chain-transform}, the remaining algebraic objective is
243
+ \eqref{eq:chain-inversion}. We next express ordinary character counts
244
+ as sums of simple-module counts in centralizers. Chain cancellation
245
+ will then replace the alternating sum of $l$ by an alternating sum of
246
+ $k_{\mathrm{ord}}$, which can be computed by central traces.
247
+
248
+ For an algebra $A$, write $V(A)=A/[A,A]$, where $[A,A]$ is the
249
+ linear span of commutators, and write $\overline a$ for the image of
250
+ $a$. A central element acts on $V(A)$ by multiplication.
251
+
252
+ Powers modulo commutators underlie K\"ulshammer's generalized Reynolds
253
+ ideals; see \cite[Section~2]{HHKM2005}. We give the finite-dimensional
254
+ argument needed to extract the two block counts.
255
+
256
+ \begin{lemma}[Cocenter ranks]\label{lem:cocenter-ranks}
257
+ For a finite-dimensional $k$-algebra $A$, the map
258
+ \[
259
+ F_A:V(A)\longrightarrow V(A),\qquad
260
+ \overline a\longmapsto\overline{a^p}
261
+ \]
262
+ is well-defined and Frobenius semilinear. Its stable image has
263
+ dimension equal to the number of simple $A$-modules, and its
264
+ summand selected by a central idempotent has dimension equal to
265
+ the corresponding simple-module count.
266
+ For $A=kX$, this stable image is the span of the $p'$-classes.
267
+ The ranks of multiplication by $E$ on that span and on all of
268
+ $V(kX)$ are, respectively, $l(X,E)$ and $k_{\mathrm{ord}}(X,E)$.
269
+ \end{lemma}
270
+
271
+ \begin{proof}
272
+ In the expansion of $(a+b)^p$, cyclic rotations of any mixed word
273
+ give the same cocenter class. Their orbits have size $p$, leaving
274
+ only $a^p$ and $b^p$. Thus the power operation into the cocenter
275
+ is additive and is Frobenius semilinear. Moreover
276
+ $\overline{(ab)^p}=\overline{(ba)^p}$, by one cyclic rotation;
277
+ additivity shows that this operation kills the linear commutator
278
+ space. It therefore descends to $F_A$.
279
+
280
+ Let $R$ be the Jacobson radical of $A$. The kernel of
281
+ $V(A)\longrightarrow V(A/R)$ is represented by elements of $R$:
282
+ lift any commutator expression downstairs and subtract it upstairs.
283
+ Since $R$ is nilpotent, a sufficiently high iterate of $F_A$ kills
284
+ this kernel. On the split semisimple algebra $A/R$, the cocenter
285
+ has one matrix-trace coordinate per simple factor, and $F_A$
286
+ raises each coordinate to the $p$th power. It is bijective because
287
+ $k$ is perfect. For example, the trace identity here follows by
288
+ triangularizing a matrix over $k$ and taking the $p$th powers of
289
+ its diagonal entries.
290
+
291
+ The descending images of $F_A$ stabilize, since they are
292
+ $k$-subspaces of a finite-dimensional space. Denote the stable image
293
+ by $S$ and the quotient map by $q:V(A)\to V(A/R)$.
294
+ Choose $m$ large enough that $S=\operatorname{im}F_A^m$ and
295
+ $F_A^m$ kills $\ker q$. On $S$, the map $F_A$ is surjective
296
+ and hence bijective, because it is semilinear for the automorphism
297
+ $a\mapsto a^p$ of the perfect field $k$. If $x\in S\cap\ker q$,
298
+ then $F_A^m(x)=0$; injectivity on $S$ gives $x=0$.
299
+ To prove surjectivity of $q|_S$, take $y\in V(A/R)$. The
300
+ Frobenius map $F_{A/R}$ is bijective, so choose $y'$ with
301
+ $F_{A/R}^m(y')=y$ and lift $y'$ to $x\in V(A)$. Then
302
+ $F_A^m(x)\in S$ and $q(F_A^m(x))=y$. Thus $q|_S$ is an
303
+ isomorphism. Finally
304
+ $(Ea)^p=Ea^p$ for a central idempotent $E$, so all these statements
305
+ respect its summand.
306
+
307
+ For a group algebra the cocenter is free on conjugacy classes,
308
+ represented by individual group elements: the commutator
309
+ relations identify exactly conjugate elements. Sufficiently high
310
+ $p$-powers land on $p'$-elements, and taking $p$th powers permutes
311
+ the $p'$-classes. This identifies the stable image. The integral
312
+ cocenter $V(\mathcal O X)$ is free on the same class basis. The
313
+ lift of $E$ projects it onto a free direct summand, whose rank is
314
+ unchanged over $k$ and $K$. Split semisimplicity over $K$ identifies
315
+ this rank with $k_{\mathrm{ord}}(X,E)$.
316
+ \end{proof}
317
+
318
+ Every group element has a unique commuting factorization into its
319
+ $p$-part and $p'$-part, both powers of that element. A
320
+ \emph{section} is the set of elements whose $p$-parts are conjugate
321
+ to a fixed $p$-element.
322
+
323
+ The next identity is Brauer's classical subsection count
324
+ \cite{Brauer1959}. The cocenter argument also proves the support
325
+ property needed for the defect-zero detector, without dividing by
326
+ class sizes in characteristic $p$.
327
+
328
+ \begin{lemma}[Subsection formula and support]\label{lem:subsections}
329
+ For every central idempotent $E\in kX$,
330
+ \begin{equation}\label{eq:subsections}
331
+ k_{\mathrm{ord}}(X,E)=
332
+ \sum_{\substack{[u]\text{ an }X\text{-class}\\u\text{ a }p\text{-element}}}
333
+ l\bigl(C_X(u),\operatorname{Br}_{\langle u\rangle}(E)\bigr).
334
+ \end{equation}
335
+ Multiplication by $E$ preserves the section decomposition of the
336
+ cocenter and the section decomposition of the center into spans
337
+ of class sums.
338
+ \end{lemma}
339
+
340
+ \begin{proof}
341
+ Fix a $p$-element $u$ and set $C=C_X(u)$. The map
342
+ $\overline t\mapsto\overline{ut}$ identifies the $p'$-class span
343
+ of $V(kC)$ with the section span belonging to $u$ in $V(kX)$.
344
+ It is a bijection of class bases: conjugacy of $ut$ and $ut'$
345
+ forces a conjugating element to centralize their common $p$-part
346
+ $u$, and the converse is immediate.
347
+
348
+ For $t\in C$ a $p'$-element, conjugation by $\langle u\rangle$
349
+ in the expansion of $Eut$ gives
350
+ \[
351
+ \overline{Eut}
352
+ =\overline{\operatorname{Br}_{\langle u\rangle}(E)ut}.
353
+ \]
354
+ Indeed, the coefficients are constant on these orbits and the
355
+ cocenter classes of their products with $ut$ agree; only fixed
356
+ orbits survive. The restricted idempotent is central in $kC$ and
357
+ preserves its $p'$-class span by \Cref{lem:cocenter-ranks}.
358
+ Multiplication by $u$ is central in $kC$, so the displayed
359
+ identification intertwines the two idempotent actions. Their ranks
360
+ are thus the terms in \eqref{eq:subsections}. Summing the ranks
361
+ over the sections proves that identity.
362
+
363
+ For the center, use the pairing
364
+ \[
365
+ Z(kX)\times V(kX)\longrightarrow k,
366
+ \qquad (a,\overline b)\longmapsto\tau(ab),
367
+ \]
368
+ where $\tau$ takes the coefficient of $1$. It is nondegenerate:
369
+ a class sum pairs with an individual representative of its inverse
370
+ class with coefficient one. Multiplication by $E$ is self-adjoint
371
+ for this pairing. Sections on the center pair with the inverse
372
+ sections of the cocenter, so preservation there proves preservation
373
+ here. In particular no class-size division is involved.
374
+ \end{proof}
375
+
376
+ \subsection{Two cancellations on chain orbits}
377
+
378
+ \begin{lemma}[Removal of nonnormal chains]\label{lem:nonnormal-cancellation}
379
+ In an alternating sum over chain orbits, every contribution that
380
+ depends only on $H_{\mathcal C}$ and $Q_r$ cancels on the nonnormal
381
+ chains. Thus such a sum may be taken over all chains or only normal
382
+ chains.
383
+ \end{lemma}
384
+
385
+ \begin{proof}
386
+ For a nonnormal chain, let $i$ be the largest index for which
387
+ $A=Q_i$ is not normal in $P=Q_r$, and let $R$ be the normal closure
388
+ of $A$ in $P$. Then $A<R\leq Q_{i+1}$: every later member is
389
+ normal in $P$. Also $R<P$. To see the latter, put the proper
390
+ subgroup $A$ in a maximal subgroup of $P$, which is normal because
391
+ $P$ is a finite $p$-group; it contains $R$.
392
+
393
+ Insert $R$ immediately after $A$ if it is absent, and remove it
394
+ if it is present. The last group $P$ and the last nonnormal member
395
+ $A$ are unchanged, so this operation is an involution. Every
396
+ element normalizing $A$ and $P$ normalizes their normal closure
397
+ $R$; hence insertion or removal leaves $H_{\mathcal C}$ unchanged.
398
+ The operation commutes with $X$-conjugation and changes the length
399
+ by one. It induces a fixed-point-free sign reversal on the orbits,
400
+ which proves cancellation.
401
+ \end{proof}
402
+
403
+ \begin{lemma}[Alternating subsection cancellation]
404
+ \label{lem:alternating-subsections}
405
+ One has
406
+ \begin{equation}\label{eq:alternating-subsections}
407
+ \sum_{\substack{\mathcal C/X\\\mathcal C\ \mathrm{normal}}}
408
+ (-1)^{|\mathcal C|}l(H_{\mathcal C},E_{\mathcal C})
409
+ =
410
+ \sum_{\substack{\mathcal C/X\\\mathcal C\ \mathrm{normal}}}
411
+ (-1)^{|\mathcal C|}k_{\mathrm{ord}}(H_{\mathcal C},E_{\mathcal C}).
412
+ \end{equation}
413
+ \end{lemma}
414
+
415
+ \begin{proof}
416
+ By \Cref{lem:nonnormal-cancellation}, both sums may be taken over
417
+ all chains. Expand the ordinary count by \Cref{lem:subsections}.
418
+ The $u=1$ terms give the simple-module sum. The other terms are
419
+ indexed by $X$-orbits of pairs $(\mathcal C,u)$, with $u\ne1$ a
420
+ $p$-element in $H_{\mathcal C}$. This orbit description follows
421
+ because the stabilizer of a fixed chain is $H_{\mathcal C}$.
422
+ The contribution of such a pair is
423
+ \begin{equation}\label{eq:pair-contribution}
424
+ l\bigl(H_{\mathcal C}\cap C_X(u),
425
+ \operatorname{Br}_{Q_r\langle u\rangle}(E)\bigr).
426
+ \end{equation}
427
+ Here $u$ normalizes $Q_r$, so $Q_r\langle u\rangle$ is a
428
+ $p$-group; successive coefficient restrictions have support
429
+ $C_X(Q_r)\cap C_X(u)=C_X(Q_r\langle u\rangle)$, proving the
430
+ idempotent in this expression.
431
+
432
+ Let $i$ be the largest index, allowing $0$ and $r$, for which
433
+ $u\notin Q_i$. Such an index exists since $Q_0=1$. Toggle
434
+ $R=Q_i\langle u\rangle$ immediately after $Q_i$: insert it
435
+ if absent, and remove it if present. It is a $p$-group, since
436
+ $u$ normalizes $Q_i$, and it is contained in every later member,
437
+ all of which contain $u$. The last member not containing $u$
438
+ therefore remains $Q_i$; this proves involutivity, including an
439
+ insertion after the terminal member and its inverse deletion.
440
+
441
+ Every element centralizing $u$ and normalizing $Q_i$ normalizes
442
+ $R$. Thus $H_{\mathcal C}\cap C_X(u)$ is unchanged. The product
443
+ of the terminal member with $\langle u\rangle$ is also unchanged,
444
+ even when the terminal member is inserted or deleted. Hence
445
+ \eqref{eq:pair-contribution} is preserved. The operation is
446
+ $X$-equivariant and reverses the sign, so all $u\ne1$ terms cancel.
447
+ \end{proof}
448
+
449
+ \subsection{Detecting defect zero by central elements}
450
+
451
+ By \Cref{lem:alternating-subsections}, it remains to prove that the
452
+ alternating ordinary-character sum in
453
+ \eqref{eq:alternating-subsections} equals $z(X,E)$. Their difference
454
+ retains the signed contributions of all characters selected by
455
+ $E_{\mathcal C}$ on positive-length normal chains, but omits the
456
+ selected defect-zero characters at the chain $(1)$. We will realize
457
+ this difference as a trace limit by constructing a central element
458
+ with the corresponding zero-or-one central-character values.
459
+
460
+ Put
461
+ \[
462
+ c_X=\sum_{u\in X\,\text{a }p\text{-element}}u,
463
+ \qquad d_X=\sum_{x,y\in X}[x,y],
464
+ \qquad I_X(a)=\sum_{x\in X}xax^{-1}.
465
+ \]
466
+ These elements and the image of $I_X$ are central. Call a block
467
+ \emph{semisimple} if its algebra is semisimple; since a block has no
468
+ nontrivial central idempotent, such a block is one full matrix
469
+ algebra over $k$.
470
+
471
+ The scalar of $d_X$ will identify these semisimple blocks with the
472
+ ordinary defect-zero characters. The complement $1-c_X$ will then remove
473
+ exactly those blocks from the central trace, using the support
474
+ information supplied by $I_X$.
475
+
476
+ The operator $I_X$ is the group-algebra Higman trace
477
+ \cite[Section~2]{Higman1955}; see also
478
+ \cite[Sections~2.4--2.5]{LorenzTokoly2011}. The use of $c_X$ to
479
+ isolate defect zero goes back to Tsushima \cite[Theorem~1]{Tsushima1971}.
480
+ The following proof records the exact radical-annihilation and
481
+ central-character consequences used in our trace limit.
482
+
483
+ \begin{lemma}[Averaging and defect zero]\label{lem:defect-zero-detection}
484
+ The image of $I_X$, and also $d_X$, annihilates the Jacobson radical
485
+ of $kX$. On a semisimple block, $d_X$ has nonzero central scalar;
486
+ on every other block its central character is zero. Each semisimple
487
+ block contains exactly one ordinary irreducible, which has defect
488
+ zero, and every ordinary defect-zero irreducible occurs in this
489
+ way. Moreover:
490
+ \begin{enumerate}[label=\textup{(\roman*)}]
491
+ \item $\operatorname{im}I_X$ is the span of class sums of elements
492
+ whose centralizers have order prime to $p$;
493
+ \item each semisimple block idempotent belongs to
494
+ $\operatorname{im}I_X$ and has zero Brauer image at every nontrivial
495
+ $p$-subgroup;
496
+ \item $\lambda_b(c_X)=0$ on every nonsemisimple block $b$.
497
+ \end{enumerate}
498
+ \end{lemma}
499
+
500
+ \begin{proof}
501
+ \textit{Radical annihilation.}
502
+ The form $(a,b)\mapsto\tau(ab)$ on $kX$ is symmetric and
503
+ nondegenerate. For dual bases $v_i,v_i^*$, the tensor
504
+ $\Omega=\sum_i v_i\otimes v_i^*$ is independent of the chosen
505
+ bases. Apply the linear map $u\otimes v\mapsto uav$ to this
506
+ tensor. In the group basis, whose dual basis consists of the inverses,
507
+ the result is $I_X(a)$. Similarly, apply
508
+ $u\otimes v\otimes w\otimes z\mapsto uwvz$ to
509
+ $\Omega\otimes\Omega$. In the group basis the result is
510
+ $\sum_{x,y\in X}xyx^{-1}y^{-1}=d_X$. Thus in any dual bases
511
+ \begin{equation}\label{eq:averaging-tensor}
512
+ I_X(a)=\sum_i v_iav_i^*,\qquad
513
+ d_X=\sum_{i,j}v_iv_jv_i^*v_j^*
514
+ =\sum_j I_X(v_j)v_j^*.
515
+ \end{equation}
516
+ For $b$ in the radical $R$, the trace identity
517
+ \[
518
+ \tau(I_X(a)b)=\operatorname{Tr}(L_bR_a)
519
+ \]
520
+ follows by writing the trace in these dual bases; $L$ and $R$
521
+ denote left and right multiplication. Since $L_b$ is nilpotent
522
+ and commutes with $R_a$, this trace is zero. Replace $b$ by $bc$
523
+ for arbitrary $c\in kX$, and use nondegeneracy to obtain
524
+ $I_X(a)b=0$. The final expression in
525
+ \eqref{eq:averaging-tensor} then shows that $d_XR=0$ as well,
526
+ because $v_j^*R\subseteq R$.
527
+
528
+ \textit{Semisimple blocks and ordinary defect zero.}
529
+ Distinct block ideals are orthogonal for the form. On a
530
+ semisimple block $M_d(k)$ its restriction is $t\operatorname{Tr}$
531
+ for some $t\in k^\times$. Indeed a symmetric functional kills
532
+ commutators, whose quotient in a matrix algebra is the trace line,
533
+ and nondegeneracy forces $t\ne0$. Matrix units $e_{ij}$ have duals
534
+ $t^{-1}e_{ji}$. Since
535
+ $\sum_{i,j}e_{ij}ae_{ji}=\operatorname{Tr}(a)1$, the first
536
+ contraction in \eqref{eq:averaging-tensor} gives
537
+ $I_X(a)=t^{-1}\operatorname{Tr}(a)1$. In particular
538
+ $I_X(e_{ij})=t^{-1}\delta_{ij}1$, so its last expression gives
539
+ \[
540
+ d_X=\sum_{i,j}I_X(e_{ij})t^{-1}e_{ji}
541
+ =t^{-2}\sum_i e_{ii}=t^{-2}1.
542
+ \]
543
+ We have therefore proved
544
+ \begin{equation}\label{eq:simple-block-scalars}
545
+ I_X(a)=t^{-1}\operatorname{Tr}(a)1,
546
+ \qquad d_X=t^{-2}1
547
+ \quad\text{on this block}.
548
+ \end{equation}
549
+ In particular its idempotent lies in the image of $I_X$; one can
550
+ take $a=te_{11}$. These formulas do not require $d$ to be nonzero
551
+ in $k$. On a nonsemisimple block, a central element with nonzero
552
+ residue scalar is a unit in its local center. Such a unit cannot
553
+ annihilate the nonzero radical. This proves the assertion about
554
+ the central character of $d_X$.
555
+
556
+ Now compute the same commutator sum in characteristic zero. If
557
+ $\chi$ has degree $d$, Schur's lemma gives
558
+ \[
559
+ \sum_{x\in X}\rho(xyx^{-1})
560
+ =\frac{|X|\chi(y)}d\,1.
561
+ \]
562
+ Multiply by $\rho(y^{-1})$, sum over $y$, and take traces.
563
+ Ordinary character orthogonality gives the scalar
564
+ \begin{equation}\label{eq:ordinary-commutator-scalar}
565
+ \lambda_\chi(d_X)=\frac{|X|^2}{\chi(1)^2}.
566
+ \end{equation}
567
+ It is integral, by the integrality of ordinary central scalars.
568
+ Its reduction is nonzero exactly when
569
+ $v_p(\chi(1))=v_p(|X|)$, namely in defect zero. The modular
570
+ calculation therefore puts exactly these characters in
571
+ semisimple blocks. Such a block has cocenter dimension one, so
572
+ \Cref{lem:cocenter-ranks} shows that its lifted block selects
573
+ exactly one ordinary irreducible. This also proves existence of
574
+ that character.
575
+
576
+ \textit{Support and the $p$-element sum.}
577
+ For a group element $g$ one has
578
+ \[
579
+ I_X(g)=|C_X(g)|\sum_{a\in[g]}a.
580
+ \]
581
+ This proves assertion (i). The support of a semisimple block
582
+ idempotent, already in this image, therefore contains no element
583
+ centralized by a nontrivial $p$-subgroup, proving (ii).
584
+
585
+ Finally fix a nontrivial $p$-subgroup $P$. Choose
586
+ $z\in Z(P)$ of order $p$. It is central also in $C_X(P)$, and
587
+ multiplication by $z$ preserves the set of $p$-elements of that
588
+ centralizer. With $q=\sum_{j=0}^{p-1}z^j$, the sum of those
589
+ $p$-elements factors as $q$ times a sum of orbit representatives.
590
+ As $q$ is central and $q^2=pq=0$, this proves
591
+ \[
592
+ \operatorname{Br}_P(c_X)^2=0,
593
+ \qquad \operatorname{Br}_P(c_X^2)=0.
594
+ \]
595
+ If $p$ divides $|C_X(g)|$, a nontrivial $p$-subgroup
596
+ $P\leq C_X(g)$ makes the coefficient of $g$ in $c_X^2$ vanish
597
+ by this identity. Assertion (i) gives $c_X^2\in\operatorname{im}I_X$.
598
+ On a nonsemisimple block its central character must therefore
599
+ vanish, by the same radical-annihilator argument. Since
600
+ $\lambda_b(c_X)^2=\lambda_b(c_X^2)=0$, assertion (iii) follows.
601
+ \end{proof}
602
+
603
+ \begin{lemma}[An element with zero-or-one residues]
604
+ \label{lem:detecting-element}
605
+ Let $v=E(1-c_X)$. It is central and supported on $p$-singular
606
+ elements. For a normal chain $\mathcal C$ of positive length, its
607
+ restriction to $H_{\mathcal C}$ satisfies
608
+ \[
609
+ \lambda_b(s_{H_{\mathcal C}}(v))=\lambda_b(E_{\mathcal C})
610
+ \in\{0,1\}
611
+ \]
612
+ for every block $b$ of $H_{\mathcal C}$. For the length-zero
613
+ chain, the scalar is one on the nonsemisimple blocks selected by
614
+ $E$ and zero on every other block.
615
+ \end{lemma}
616
+
617
+ \begin{proof}
618
+ The element $1-c_X$ is the negative sum of the nonidentity
619
+ $p$-elements, hence lies entirely in $p$-singular sections.
620
+ Section preservation from \Cref{lem:subsections} proves the same
621
+ support assertion for $v$. Let $B_0$ be a semisimple block
622
+ idempotent. Since $v$ is central and $B_0kX$ is a full matrix
623
+ algebra, $B_0v$ lies in its one-dimensional center $kB_0$.
624
+ On the other hand, section preservation makes the support of $B_0v$
625
+ $p$-singular. By \Cref{lem:defect-zero-detection}, the support
626
+ of $B_0$ contains only elements whose centralizers have order prime
627
+ to $p$, and therefore no $p$-singular elements. The two support
628
+ conditions force the scalar multiple $B_0v$ to be zero.
629
+ On a nonsemisimple block,
630
+ \Cref{lem:defect-zero-detection} gives
631
+ $\lambda_b(v)=\lambda_b(E)$, proving the length-zero assertion.
632
+
633
+ For positive length, put $Q=Q_r\ne1$ and $H=H_{\mathcal C}$.
634
+ By \Cref{lem:normalizer-projection}, $\lambda_b\circ s_H$ is a
635
+ central character of $X$ and factors through
636
+ $\operatorname{Br}_Q$. It cannot be the character of a
637
+ semisimple block $B_0$: that would give value one on $B_0$,
638
+ whereas $\operatorname{Br}_Q(B_0)=0$ by
639
+ \Cref{lem:defect-zero-detection}. On its nonsemisimple block,
640
+ $\lambda(v)=\lambda(E)$. Applying
641
+ \Cref{lem:normalizer-projection} to $E$ gives the asserted value
642
+ $\lambda_b(E_{\mathcal C})$.
643
+ \end{proof}
644
+
645
+ \subsection{Central traces and the final cancellation}
646
+
647
+ Choose a class-sum lift
648
+ \[
649
+ \widehat v=\sum_{a\in X}\alpha_a a\in Z(\mathcal O X)
650
+ \]
651
+ of the detecting element $v=E(1-c_X)$ from
652
+ \Cref{lem:detecting-element}, with $\alpha_a=0$ whenever $a$ is
653
+ not $p$-singular.
654
+ For a positive integer $n$, define
655
+ \begin{equation}\label{eq:chain-trace}
656
+ \Phi_n=
657
+ \sum_{\mathcal C/X}(-1)^{|\mathcal C|}
658
+ \operatorname{Tr}\left(
659
+ s_{H_{\mathcal C}}(\widehat v)^n
660
+ \mid V(KH_{\mathcal C})\right),
661
+ \end{equation}
662
+ where the operator is central multiplication and all chains are
663
+ included.
664
+
665
+ \begin{lemma}[The first trace limit]\label{lem:trace-limit}
666
+ In the valuation topology of $K$,
667
+ \begin{equation}\label{eq:trace-limit}
668
+ \lim_{s\to\infty}\Phi_{p^s}
669
+ =
670
+ \sum_{\substack{\mathcal C/X\\\mathcal C\ \mathrm{normal}}}
671
+ (-1)^{|\mathcal C|}k_{\mathrm{ord}}(H_{\mathcal C},E_{\mathcal C})
672
+ -z(X,E).
673
+ \end{equation}
674
+ \end{lemma}
675
+
676
+ \begin{proof}
677
+ The nonnormal chains cancel by
678
+ \Cref{lem:nonnormal-cancellation}, since their trace contribution
679
+ depends only on the stabilizer. For a remaining chain, the
680
+ cocenter of $KH_{\mathcal C}$ has one coordinate per ordinary
681
+ irreducible. The unpowered operator has on these coordinates
682
+ integral central eigenvalues reducing to the scalars in
683
+ \Cref{lem:detecting-element}.
684
+
685
+ If an eigenvalue reduces to zero, its $p^s$th powers tend to zero.
686
+ If it is $1+a$ with $\operatorname{val}(a)>0$, the binomial
687
+ formula gives
688
+ \[
689
+ \operatorname{val}((1+a)^p-1)
690
+ \geq
691
+ \min\{\operatorname{val}(p)+\operatorname{val}(a),
692
+ p\operatorname{val}(a)\}.
693
+ \]
694
+ After normalizing the discrete valuation to integer values, each
695
+ iteration increases the positive valuation by at least one, unless
696
+ the difference has already become zero. These powers tend to one.
697
+ This argument applies also to $p=2$ and requires no finiteness of
698
+ the residue field.
699
+
700
+ For positive-length chains the limiting trace therefore counts
701
+ all ordinary irreducibles selected by $E_{\mathcal C}$. At length
702
+ zero it omits the semisimple blocks, each of which contributes
703
+ exactly one defect-zero character by
704
+ \Cref{lem:defect-zero-detection}. There are finitely many chains
705
+ and irreducibles, so limits may be summed, proving
706
+ \eqref{eq:trace-limit}.
707
+ \end{proof}
708
+
709
+ The next identity follows from Frobenius's commutator-counting formula
710
+ and is the weighted genus-one case of the surface formula in
711
+ \cite[Theorem~2.1 and Equation~(3.1)]{Klug2025}. Its single
712
+ denominator is important when chain orbits are replaced by actual
713
+ chains, so we verify the normalization directly.
714
+
715
+ \begin{lemma}[Trace normalization]\label{lem:tuple-trace}
716
+ For $H\leq X$ and $w=s_H(\widehat v)$,
717
+ \begin{equation}\label{eq:tuple-trace}
718
+ \operatorname{Tr}(w^n\mid V(KH))
719
+ =\frac1{|H|}
720
+ \sum_{\substack{x,y,u_1,\ldots,u_n\in H\\
721
+ [x,y]u_1\cdots u_n=1}}
722
+ \prod_{i=1}^n\alpha_{u_i}.
723
+ \end{equation}
724
+ \end{lemma}
725
+
726
+ \begin{proof}
727
+ The sum on the right before division is
728
+ $\tau(d_Hw^n)$. The regular trace of any element of $KH$ is
729
+ $|H|$ times its identity coefficient. On the other hand,
730
+ \eqref{eq:ordinary-commutator-scalar} and the regular decomposition
731
+ give
732
+ \begin{align*}
733
+ |H|\tau(d_Hw^n)
734
+ &=\sum_{\chi\in\operatorname{Irr}(H)}
735
+ \chi(1)^2\frac{|H|^2}{\chi(1)^2}\lambda_\chi(w)^n\\
736
+ &=|H|^2\operatorname{Tr}(w^n\mid V(KH)).
737
+ \end{align*}
738
+ Dividing proves exactly the single denominator in
739
+ \eqref{eq:tuple-trace}.
740
+ \end{proof}
741
+
742
+ For a subgroup $J\leq X$, define an integer on actual chains,
743
+ without quotienting by conjugation,
744
+ \begin{equation}\label{eq:chain-weight}
745
+ a_X(J)=
746
+ \sum_{\substack{\mathcal C\text{ a chain in }X\\
747
+ J\leq H_{\mathcal C}}}(-1)^{|\mathcal C|}.
748
+ \end{equation}
749
+
750
+ \begin{lemma}[Cancellation by a normal $p$-subgroup]
751
+ \label{lem:pcore-cancellation}
752
+ If $O_p(J)\ne1$, then $a_X(J)=0$.
753
+ \end{lemma}
754
+
755
+ \begin{proof}
756
+ Put $P=O_p(J)$. In any chain normalized by $J$, each $Q_i$ is
757
+ normalized by $P\leq J$, so $Q_iP$ is a $p$-subgroup. Both
758
+ factors are normalized by $J$, making their product
759
+ $J$-normalized. Let $i$ be the last index such that $P\nleq Q_i$;
760
+ it exists since $Q_0=1$ and $P\ne1$. Toggle $Q_iP$ immediately
761
+ after $Q_i$. It strictly contains $Q_i$ and is contained in all
762
+ later members. Insertion and deletion preserve the last member
763
+ not containing $P$, so this is an involution. It is defined also
764
+ for the length-zero chain and for terminal insertion or deletion.
765
+ It preserves the property of being normalized by $J$ and reverses
766
+ the sign. The sum of actual chains in \eqref{eq:chain-weight}
767
+ therefore vanishes.
768
+ \end{proof}
769
+
770
+ \begin{proposition}[Reduction to uniform tuple divisibility]
771
+ \label{prop:group-reduction}
772
+ If \Cref{thm:tuple-divisibility} holds for every finite group with
773
+ trivial $p$-core, then for every finite group $X$ and central
774
+ idempotent $E\in kX$ one has $l(X,E)=((1+T)z)(X,E)$.
775
+ In particular the block equality in \Cref{thm:main} follows, with
776
+ the stated block assignment and with $Q=1$ included.
777
+ \end{proposition}
778
+
779
+ \begin{proof}
780
+ The orbit of a chain $\mathcal C$ has size
781
+ $|X|/|H_{\mathcal C}|$. Consequently
782
+ \Cref{lem:tuple-trace} changes the orbit sum
783
+ \eqref{eq:chain-trace} into the following sum over actual tuples
784
+ and actual chains:
785
+ \begin{equation}\label{eq:trace-by-generated-group}
786
+ \Phi_n=\frac1{|X|}
787
+ \sum_{\substack{x,y,u_1,\ldots,u_n\in X\\
788
+ [x,y]u_1\cdots u_n=1}}
789
+ a_X\bigl(\langle x,y,u_1,\ldots,u_n\rangle\bigr)
790
+ \prod_{i=1}^n\alpha_{u_i}.
791
+ \end{equation}
792
+ To verify the factor, each orbit contribution has prefactor
793
+ $1/|H_{\mathcal C}|$; replacing its representative by all
794
+ $|X|/|H_{\mathcal C}|$ conjugates gives the common prefactor
795
+ $1/|X|$. For a fixed tuple the admissible chains are exactly those
796
+ normalized by its generated subgroup. This is precisely
797
+ $a_X(J)$.
798
+
799
+ By \Cref{lem:pcore-cancellation}, only generated subgroups
800
+ $J$ with $O_p(J)=1$ contribute. By the support of $\widehat v$,
801
+ only tuples with every $u_i$ $p$-singular contribute. Fix such a
802
+ subgroup $J$ and group its generating tuples according to the
803
+ multiset $\mathcal M$ of $J$-conjugacy classes of the $u_i$.
804
+ The product $\prod_i\alpha_{u_i}$ is constant on this multiset:
805
+ the coefficients are constant on $X$-classes, hence on $J$-classes,
806
+ and their product is unchanged by reordering. Denote this integral
807
+ product by $\alpha(\mathcal M)$. A generating tuple has simultaneous
808
+ conjugation stabilizer $Z(J)$, since an element centralizing all
809
+ its entries centralizes the group they generate. Thus its number
810
+ of actual tuples is $|J|/|Z(J)|$ times its orbit count. For
811
+ $n=p^s$, the numerator in \eqref{eq:trace-by-generated-group}
812
+ is therefore
813
+ \begin{equation}\label{eq:uniform-numerator}
814
+ \sum_{\substack{J\leq X\\O_p(J)=1}}
815
+ a_X(J)\frac{|J|}{|Z(J)|}
816
+ \sum_{\mathcal M}
817
+ \alpha(\mathcal M)N_{J,s}(\mathcal M).
818
+ \end{equation}
819
+
820
+ Fix any $h\geq1$. By \Cref{thm:tuple-divisibility}, each summand
821
+ of the inner sum belongs to $p^h\mathcal O$ for all sufficiently
822
+ large $s$, with a threshold independent of $\mathcal M$. Although
823
+ the number of multisets grows with $s$, the sum is finite for each
824
+ $s$ and remains in that same ideal. There are only finitely many
825
+ subgroups $J\leq X$, so take the largest of their thresholds.
826
+ The integer factors in \eqref{eq:uniform-numerator} preserve
827
+ divisibility. We conclude that its numerator tends to zero in the
828
+ valuation topology. The fixed denominator $|X|$ does not change
829
+ this conclusion, so $\Phi_{p^s}\longrightarrow0$.
830
+
831
+ Combine this with \Cref{lem:trace-limit} and
832
+ \Cref{lem:alternating-subsections}. The resulting equality is
833
+ \eqref{eq:chain-inversion}; its integer terms agree in the
834
+ characteristic-zero field $K$, and hence agree as integers.
835
+ The same reasoning applies to every pair and to the splitting
836
+ subquotients arising in the transform. \Cref{lem:chain-transform}
837
+ now gives $l=(1+T)z$. The weight interpretation of
838
+ \eqref{eq:weight-transform} proves the asserted block equality.
839
+ \end{proof}