import Mathlib.Algebra.Field.ZMod import Mathlib.LinearAlgebra.Dimension.Constructions import Mathlib.LinearAlgebra.FiniteDimensional.Basic import Mathlib.LinearAlgebra.FiniteDimensional.Lemmas import Mathlib.LinearAlgebra.Prod import Mathlib.Order.ModularLattice import Mathlib.Tactic.Abel namespace OAI section /-! Complements adapted to an affine restriction. The prescribed directions are contained in a small summand, and the complementary directions are mapped into the prescribed target subspace. This is ordinary finite-dimensional geometry; no Fourier inequality or pseudorandomness hypothesis is used. -/ namespace UniqueGamesTheorem.Inverse.KMSAffineRestrictionComplement variable {K E F : Type*} [DivisionRing K] [AddCommGroup E] [Module K E] [FiniteDimensional K E] [AddCommGroup F] [Module K F] /-- Enlarge prescribed directions by at most the rank of `L`, leaving a complement on which `L` vanishes. -/ theorem exists_bounded_complement_of_linearMap (V1 : Submodule K E) (L : E →ₗ[K] F) : ∃ U E0 : Submodule K E, V1 ≤ U ∧ E0 ≤ LinearMap.ker L ∧ IsCompl U E0 ∧ Module.finrank K U ≤ Module.finrank K V1 + Module.finrank K (LinearMap.range L) := by obtain ⟨D, hD⟩ := (LinearMap.ker L).exists_isCompl let U : Submodule K E := V1 ⊔ D have hcover : Codisjoint (LinearMap.ker L) U := hD.codisjoint.mono_right le_sup_right obtain ⟨E0, hE0, hcompl⟩ := hcover.exists_isCompl refine ⟨U, E0, le_sup_left, hE0, hcompl.symm, ?_⟩ have hdim := Submodule.finrank_add_eq_of_isCompl hD have hrank := LinearMap.finrank_range_add_finrank_ker L have hDdim : Module.finrank K D = Module.finrank K (LinearMap.range L) := by omega exact (Submodule.finrank_add_le_finrank_add_finrank V1 D).trans (by rw [hDdim]) /-- Split the domain while preserving `V1` and mapping all complementary directions into `W`. The extra dimension is at most the codimension of `W`. -/ theorem exists_bounded_complement [FiniteDimensional K F] (V1 : Submodule K E) (W : Submodule K F) (T : E →ₗ[K] F) : ∃ U E0 : Submodule K E, V1 ≤ U ∧ E0 ≤ LinearMap.ker (W.mkQ.comp T) ∧ IsCompl U E0 ∧ Module.finrank K U ≤ Module.finrank K V1 + Module.finrank K (F ⧸ W) := by obtain ⟨U, E0, hV1, hE0, hcompl, hdim⟩ := exists_bounded_complement_of_linearMap V1 (W.mkQ.comp T) refine ⟨U, E0, hV1, hE0, hcompl, hdim.trans ?_⟩ exact Nat.add_le_add_left (Submodule.finrank_le (LinearMap.range (W.mkQ.comp T))) _ end UniqueGamesTheorem.Inverse.KMSAffineRestrictionComplement end section /-! An explicit splitting of a linear functional with a chosen unit preimage. Both directions retain the chosen vector, permitting compatible splittings of nested spaces and subspaces in the KMS argument. -/ namespace UniqueGamesTheorem.Inverse.KMSAnalyticFunctionalSplit variable {K F : Type*} [Field K] [AddCommGroup F] [Module K F] /-- Split off the coordinate measured by `a`, using the prescribed vector `t`. The kernel coordinate is exactly `x - a x • t`. -/ def splitEquiv (a : F →ₗ[K] K) (t : F) (ht : a t = 1) : F ≃ₗ[K] (a.ker × K) where toFun x := (⟨x - a x • t, by simp [LinearMap.mem_ker, ht]⟩, a x) invFun p := (p.1 : F) + p.2 • t map_add' x y := by apply Prod.ext · apply Subtype.ext change x + y - a (x + y) • t = (x - a x • t) + (y - a y • t) rw [map_add, add_smul] abel · exact a.map_add x y map_smul' c x := by apply Prod.ext · apply Subtype.ext change c • x - a (c • x) • t = c • (x - a x • t) simp [smul_sub, smul_smul] · exact a.map_smul c x left_inv x := by change x - a x • t + a x • t = x exact sub_add_cancel _ _ right_inv p := by have hp : a (p.1 : F) = 0 := p.1.property apply Prod.ext · apply Subtype.ext change (p.1 : F) + p.2 • t - a ((p.1 : F) + p.2 • t) • t = p.1 simp [hp, ht] · change a ((p.1 : F) + p.2 • t) = p.2 simp [hp, ht] @[simp] theorem splitEquiv_apply_snd (a : F →ₗ[K] K) (t : F) (ht : a t = 1) (x : F) : (splitEquiv a t ht x).2 = a x := rfl @[simp] theorem splitEquiv_apply_fst_coe (a : F →ₗ[K] K) (t : F) (ht : a t = 1) (x : F) : ((splitEquiv a t ht x).1 : F) = x - a x • t := rfl @[simp] theorem splitEquiv_symm_apply (a : F →ₗ[K] K) (t : F) (ht : a t = 1) (p : a.ker × K) : (splitEquiv a t ht).symm p = (p.1 : F) + p.2 • t := rfl @[simp] theorem splitEquiv_symm_apply_zero (a : F →ₗ[K] K) (t : F) (ht : a t = 1) (b : a.ker) : (splitEquiv a t ht).symm (b, 0) = (b : F) := by simp @[simp] theorem splitEquiv_apply_ker (a : F →ₗ[K] K) (t : F) (ht : a t = 1) (b : a.ker) : splitEquiv a t ht (b : F) = (b, 0) := by apply (splitEquiv a t ht).symm.injective simp @[simp] theorem splitEquiv_apply_unit (a : F →ₗ[K] K) (t : F) (ht : a t = 1) : splitEquiv a t ht t = (0, 1) := by apply (splitEquiv a t ht).symm.injective simp /-- A functional with a unit preimage has a kernel of codimension one. -/ theorem finrank_eq_ker_add_one [FiniteDimensional K F] (a : F →ₗ[K] K) (t : F) (ht : a t = 1) : Module.finrank K F = Module.finrank K a.ker + 1 := by have h := (splitEquiv a t ht).finrank_eq simpa [Module.finrank_prod] using h end UniqueGamesTheorem.Inverse.KMSAnalyticFunctionalSplit end section /-! Compatible one-coordinate splittings of two surjections with a common target. A single target coordinate is lifted through both maps. The three resulting linear equivalences put both surjections into the product of their kernel restriction with the identity on the binary field. -/ namespace UniqueGamesTheorem.Inverse.KMSAnalyticCompatibleSplitting noncomputable section abbrev F2 := ZMod 2 variable {I F K : Type*} [AddCommGroup I] [Module F2 I] [AddCommGroup F] [Module F2 F] [AddCommGroup K] [Module F2 K] /-- Data of one common coordinate and compatible section vectors. All maps and all smaller spaces below are constructed from these original data. -/ structure CompatibleSplitting (π : I →ₗ[F2] K) (A : F →ₗ[F2] K) where functional : K →ₗ[F2] F2 targetVector : K functional_targetVector : functional targetVector = 1 leftVector : I leftVector_image : π leftVector = targetVector rightVector : F rightVector_image : A rightVector = targetVector left_surjective : Function.Surjective π right_surjective : Function.Surjective A namespace CompatibleSplitting variable {π : I →ₗ[F2] K} {A : F →ₗ[F2] K} abbrev K0 (s : CompatibleSplitting π A) := s.functional.ker abbrev J (s : CompatibleSplitting π A) := (s.functional.comp π).ker abbrev B (s : CompatibleSplitting π A) := (s.functional.comp A).ker def targetEquiv (s : CompatibleSplitting π A) : K ≃ₗ[F2] (s.K0 × F2) := KMSAnalyticFunctionalSplit.splitEquiv s.functional s.targetVector s.functional_targetVector def leftEquiv (s : CompatibleSplitting π A) : I ≃ₗ[F2] (s.J × F2) := KMSAnalyticFunctionalSplit.splitEquiv (s.functional.comp π) s.leftVector (by change s.functional (π s.leftVector) = 1 rw [s.leftVector_image, s.functional_targetVector]) def rightEquiv (s : CompatibleSplitting π A) : F ≃ₗ[F2] (s.B × F2) := KMSAnalyticFunctionalSplit.splitEquiv (s.functional.comp A) s.rightVector (by change s.functional (A s.rightVector) = 1 rw [s.rightVector_image, s.functional_targetVector]) /-- The remaining part of the left surjection is its literal restriction. -/ def leftMap (s : CompatibleSplitting π A) : s.J →ₗ[F2] s.K0 := (π.comp (s.functional.comp π).ker.subtype).codRestrict s.functional.ker (fun x => x.property) /-- The remaining part of the right surjection is its literal restriction. -/ def rightMap (s : CompatibleSplitting π A) : s.B →ₗ[F2] s.K0 := (A.comp (s.functional.comp A).ker.subtype).codRestrict s.functional.ker (fun x => x.property) @[simp] theorem leftMap_apply_val (s : CompatibleSplitting π A) (x : s.J) : (s.leftMap x : K) = π x := rfl @[simp] theorem rightMap_apply_val (s : CompatibleSplitting π A) (x : s.B) : (s.rightMap x : K) = A x := rfl theorem leftMap_surjective (s : CompatibleSplitting π A) : Function.Surjective s.leftMap := by intro y obtain ⟨x, hx⟩ := s.left_surjective y.val refine ⟨⟨x, ?_⟩, ?_⟩ · change s.functional (π x) = 0 rw [hx] exact y.property · apply Subtype.ext exact hx theorem rightMap_surjective (s : CompatibleSplitting π A) : Function.Surjective s.rightMap := by intro y obtain ⟨x, hx⟩ := s.right_surjective y.val refine ⟨⟨x, ?_⟩, ?_⟩ · change s.functional (A x) = 0 rw [hx] exact y.property · apply Subtype.ext exact hx @[simp] theorem leftEquiv_symm_apply (s : CompatibleSplitting π A) (x : s.J × F2) : s.leftEquiv.symm x = (x.1 : I) + x.2 • s.leftVector := rfl @[simp] theorem rightEquiv_symm_apply (s : CompatibleSplitting π A) (x : s.B × F2) : s.rightEquiv.symm x = (x.1 : F) + x.2 • s.rightVector := rfl @[simp] theorem targetEquiv_symm_apply (s : CompatibleSplitting π A) (x : s.K0 × F2) : s.targetEquiv.symm x = (x.1 : K) + x.2 • s.targetVector := rfl theorem left_symm_apply (s : CompatibleSplitting π A) (x : s.J × F2) : π (s.leftEquiv.symm x) = s.targetEquiv.symm (s.leftMap x.1, x.2) := by change π ((x.1 : I) + x.2 • s.leftVector) = π x.1 + x.2 • s.targetVector rw [map_add, map_smul, s.leftVector_image] theorem right_symm_apply (s : CompatibleSplitting π A) (x : s.B × F2) : A (s.rightEquiv.symm x) = s.targetEquiv.symm (s.rightMap x.1, x.2) := by change A ((x.1 : F) + x.2 • s.rightVector) = A x.1 + x.2 • s.targetVector rw [map_add, map_smul, s.rightVector_image] /-- Both changes of coordinates use the same final binary coordinate. -/ theorem left_conjugation (s : CompatibleSplitting π A) : s.targetEquiv.toLinearMap.comp (π.comp s.leftEquiv.symm.toLinearMap) = s.leftMap.prodMap (LinearMap.id : F2 →ₗ[F2] F2) := by apply LinearMap.ext intro x change s.targetEquiv (π (s.leftEquiv.symm x)) = (s.leftMap x.1, x.2) rw [s.left_symm_apply, s.targetEquiv.apply_symm_apply] theorem right_conjugation (s : CompatibleSplitting π A) : s.targetEquiv.toLinearMap.comp (A.comp s.rightEquiv.symm.toLinearMap) = s.rightMap.prodMap (LinearMap.id : F2 →ₗ[F2] F2) := by apply LinearMap.ext intro x change s.targetEquiv (A (s.rightEquiv.symm x)) = (s.rightMap x.1, x.2) rw [s.right_symm_apply, s.targetEquiv.apply_symm_apply] theorem target_finrank [FiniteDimensional F2 K] (s : CompatibleSplitting π A) : Module.finrank F2 K = Module.finrank F2 s.K0 + 1 := KMSAnalyticFunctionalSplit.finrank_eq_ker_add_one s.functional s.targetVector s.functional_targetVector theorem left_finrank [FiniteDimensional F2 I] (s : CompatibleSplitting π A) : Module.finrank F2 I = Module.finrank F2 s.J + 1 := KMSAnalyticFunctionalSplit.finrank_eq_ker_add_one (s.functional.comp π) s.leftVector (by change s.functional (π s.leftVector) = 1 rw [s.leftVector_image, s.functional_targetVector]) theorem right_finrank [FiniteDimensional F2 F] (s : CompatibleSplitting π A) : Module.finrank F2 F = Module.finrank F2 s.B + 1 := KMSAnalyticFunctionalSplit.finrank_eq_ker_add_one (s.functional.comp A) s.rightVector (by change s.functional (A s.rightVector) = 1 rw [s.rightVector_image, s.functional_targetVector]) end CompatibleSplitting /-- Positive target dimension supplies a basis coordinate; surjectivity supplies its two lifts. No additional splitting hypothesis is required. -/ theorem exists_compatibleSplitting [FiniteDimensional F2 K] (π : I →ₗ[F2] K) (A : F →ₗ[F2] K) (hπ : Function.Surjective π) (hA : Function.Surjective A) (hdim : 0 < Module.finrank F2 K) : Nonempty (CompatibleSplitting π A) := by classical let b := Module.finBasis F2 K let j : Fin (Module.finrank F2 K) := ⟨0, hdim⟩ obtain ⟨i, hi⟩ := hπ (b j) obtain ⟨f, hf⟩ := hA (b j) refine ⟨⟨b.coord j, b j, ?_, i, hi, f, hf, hπ, hA⟩⟩ simp def chooseSplit [FiniteDimensional F2 K] (π : I →ₗ[F2] K) (A : F →ₗ[F2] K) (hπ : Function.Surjective π) (hA : Function.Surjective A) (hdim : 0 < Module.finrank F2 K) : CompatibleSplitting π A := Classical.choice (exists_compatibleSplitting π A hπ hA hdim) end end UniqueGamesTheorem.Inverse.KMSAnalyticCompatibleSplitting end section namespace UniqueGamesTheorem.Inverse.KMSAnalyticHybridCoordinates variable {R A W D B C : Type*} [Ring R] [AddCommGroup A] [Module R A] [AddCommGroup W] [Module R W] [AddCommGroup D] [Module R D] [AddCommGroup B] [Module R B] [AddCommGroup C] [Module R C] /-- The chosen block compression: restrict to `B`, then forget `A`. -/ def compressBlock (S : (B × C) →ₗ[R] (A × (W × D))) : B →ₗ[R] (W × D) := (LinearMap.snd R A (W × D)).comp (S.comp (LinearMap.inl R B C)) @[simp] theorem compressBlock_apply (S : (B × C) →ₗ[R] (A × (W × D))) (b : B) : compressBlock S b = (S (b, 0)).2 := rfl /-- Coordinates of a map whose compression is `(z,0)`. -/ structure Coordinates (z : B →ₗ[R] W) where alpha : (B × C) →ₗ[R] A psi : (B × C) →ₗ[R] W psi_left : psi.comp (LinearMap.inl R B C) = z v : C →ₗ[R] D @[ext] theorem Coordinates.ext {z : B →ₗ[R] W} {p q : Coordinates (A := A) (D := D) (C := C) z} (ha : p.alpha = q.alpha) (hp : p.psi = q.psi) (hv : p.v = q.v) : p = q := by cases p cases q cases ha cases hp cases hv rfl /-- Assemble the three blocks. The last coordinate vanishes on `B`. -/ def assemble {z : B →ₗ[R] W} (p : Coordinates (A := A) (D := D) (C := C) z) : (B × C) →ₗ[R] (A × (W × D)) := p.alpha.prod (p.psi.prod (p.v.comp (LinearMap.snd R B C))) @[simp] theorem assemble_apply {z : B →ₗ[R] W} (p : Coordinates (A := A) (D := D) (C := C) z) (x : B × C) : assemble p x = (p.alpha x, p.psi x, p.v x.2) := rfl @[simp] theorem compressBlock_assemble {z : B →ₗ[R] W} (p : Coordinates (A := A) (D := D) (C := C) z) : compressBlock (assemble p) = z.prod (0 : B →ₗ[R] D) := by apply LinearMap.ext intro b have hp : p.psi (b, 0) = z b := congrArg (fun L : (B →ₗ[R] W) => L b) p.psi_left simp [compressBlock, assemble, hp] /-- Extract the unique coordinates from an actual compressed-fiber element. -/ def extract (z : B →ₗ[R] W) (S : {S : (B × C) →ₗ[R] (A × (W × D)) // compressBlock S = z.prod (0 : B →ₗ[R] D)}) : Coordinates (A := A) (D := D) (C := C) z where alpha := (LinearMap.fst R A (W × D)).comp S.val psi := (LinearMap.fst R W D).comp ((LinearMap.snd R A (W × D)).comp S.val) psi_left := by apply LinearMap.ext intro b exact congrArg (fun L : B →ₗ[R] (W × D) => (L b).1) S.property v := (LinearMap.snd R W D).comp ((LinearMap.snd R A (W × D)).comp (S.val.comp (LinearMap.inr R B C))) @[simp] theorem assemble_extract (z : B →ₗ[R] W) (S : {S : (B × C) →ₗ[R] (A × (W × D)) // compressBlock S = z.prod (0 : B →ₗ[R] D)}) : assemble (extract z S) = S.val := by apply LinearMap.ext rintro ⟨b, c⟩ have hzero : (S.val (b, 0)).2.2 = 0 := congrArg (fun L : B →ₗ[R] (W × D) => (L b).2) S.property have hlast : (S.val (b, c)).2.2 = (S.val (0, c)).2.2 := by calc _ = (S.val ((b, 0) + (0, c))).2.2 := by simp _ = (S.val (b, 0)).2.2 + (S.val (0, c)).2.2 := by rw [map_add]; rfl _ = _ := by rw [hzero, zero_add] apply Prod.ext · rfl · apply Prod.ext · rfl · exact hlast.symm @[simp] theorem extract_assemble {z : B →ₗ[R] W} (p : Coordinates (A := A) (D := D) (C := C) z) : extract z ⟨assemble p, compressBlock_assemble p⟩ = p := by apply Coordinates.ext · apply LinearMap.ext intro x rfl · apply LinearMap.ext intro x rfl · apply LinearMap.ext intro c rfl /-- An exact compressed-fiber parametrization, valid over any ring. -/ def compressedFiberEquiv (z : B →ₗ[R] W) : {S : (B × C) →ₗ[R] (A × (W × D)) // compressBlock S = z.prod (0 : B →ₗ[R] D)} ≃ Coordinates (A := A) (D := D) (C := C) z where toFun := extract z invFun p := ⟨assemble p, compressBlock_assemble p⟩ left_inv S := Subtype.ext (assemble_extract z S) right_inv := extract_assemble /-- Equality of assembled maps forces equality of every chosen coordinate; there are no hidden change-of-basis fibers in this parametrization. -/ theorem assemble_injective (z : B →ₗ[R] W) : Function.Injective (assemble (R := R) (A := A) (D := D) (C := C) (z := z)) := by intro p q h have hh : (compressedFiberEquiv (A := A) (D := D) (C := C) z).symm p = (compressedFiberEquiv (A := A) (D := D) (C := C) z).symm q := Subtype.ext h exact (compressedFiberEquiv (A := A) (D := D) (C := C) z).symm.injective hh end UniqueGamesTheorem.Inverse.KMSAnalyticHybridCoordinates end end OAI