import OAI.Analysis.Cuntz.RegularizedState import Mathlib.MeasureTheory.Integral.IntervalIntegral.Basic namespace OAI noncomputable section /-! Spectral distributions, integrals, and scalar covariance. -/ open scoped Matrix CStarAlgebra open MeasureTheory namespace Kaplansky attribute [local instance] CStarAlgebra.spectralOrder CStarAlgebra.spectralOrderedRing variable {A : Type*} [CStarAlgebra A] /-- A positive cutoff vanishes above the actual spectral norm bound. -/ theorem cuntzCutoff_eq_zero_of_norm_le {a : A} (ha : 0 ≤ a) {ε : ℝ} (hε : ‖a‖ ≤ ε) : cuntzCutoff a ε = 0 := by nontriviality A change cfc (fun t : ℝ => max (t-ε) 0) a = 0 rw [← cfc_zero ℝ a] apply cfc_congr intro t ht have h : t ≤ ε := by simpa only [Real.norm_of_nonneg (spectrum_nonneg_of_nonneg ha ht)] using (spectrum.norm_le_norm_of_mem ht).trans hε exact max_eq_right (sub_nonpos.mpr h) theorem cuntzCutoff_one_of_lt {t : ℝ} (ht : t < 1) : cuntzCutoff (1 : A) t = (1 - t) • (1 : A) := by have h := cfc_algebraMap (A := A) (1 : ℝ) (fun x : ℝ => max (x - t) 0) simpa only [cuntzCutoff, map_one, max_eq_left (sub_nonneg.mpr ht.le), Algebra.algebraMap_eq_smul_one] using h namespace CuntzDimensionState theorem regularized_of_matrix_eq_zero (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) (ha : a.matrix = 0) : d.regularized a = 0 := by rw [← d.regularized_zero] apply d.regularized_eq change CuntzEquivalent a.matrix (0 : Matrix (Fin 0) (Fin 0) A) rw [ha] exact ⟨CuntzLE.zero _, CuntzLE.zero _⟩ /-- The regularized spectral distribution attached to an actual positive matrix. -/ def distribution (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) (t : ℝ) : ℝ := d.regularized (a.cutoff t) theorem distribution_antitone (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) : Antitone (d.distribution a) := by intro s t h exact d.regularized_mono (a := a.cutoff t) (b := a.cutoff s) (cuntzLE_of_nonneg_le (cuntzCutoff_nonneg _ _) (cuntzCutoff_antitone _ h)) theorem distribution_nonneg (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) (t : ℝ) : 0 ≤ d.distribution a t := d.regularized_nonneg _ theorem distribution_le_size (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) (t : ℝ) : d.distribution a t ≤ a.size := d.regularized_le_size _ theorem distribution_eq_zero (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) {t : ℝ} (ht : ‖CStarMatrix.ofMatrix a.matrix‖ ≤ t) : d.distribution a t = 0 := by apply d.regularized_of_matrix_eq_zero change CStarMatrix.ofMatrix.symm (cuntzCutoff (CStarMatrix.ofMatrix a.matrix) t) = 0 rw [cuntzCutoff_eq_zero_of_norm_le a.nonneg ht] rfl theorem distribution_intervalIntegrable (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) (s t : ℝ) : IntervalIntegrable (d.distribution a) volume s t := (d.distribution_antitone a).intervalIntegrable theorem distribution_add (d : CuntzDimensionState A) (a b : CuntzPositiveMatrix A) (t : ℝ) : d.distribution (a.add b) t = d.distribution a t + d.distribution b t := by simp only [distribution, CuntzPositiveMatrix.cutoff_add, d.regularized_add] /-- Finite layer-cake integral. This definition does not assert the quasitrace axioms. -/ def spectralValue (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) : ℝ := ∫ t in (0 : ℝ)..‖CStarMatrix.ofMatrix a.matrix‖, d.distribution a t theorem spectralValue_nonneg (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) : 0 ≤ d.spectralValue a := intervalIntegral.integral_nonneg_of_forall (norm_nonneg _) (d.distribution_nonneg a) theorem spectralValue_le_norm_mul_size (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) : d.spectralValue a ≤ ‖CStarMatrix.ofMatrix a.matrix‖ * a.size := by have h := intervalIntegral.integral_mono_on (norm_nonneg (CStarMatrix.ofMatrix a.matrix)) (d.distribution_intervalIntegrable a 0 _) intervalIntegrable_const (fun t _ => d.distribution_le_size a t) simpa only [spectralValue, intervalIntegral.integral_const, sub_zero, smul_eq_mul] using h /-- The layer-cake integral is independent of an upper endpoint past the norm. -/ theorem spectralValue_eq_integral (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) {R : ℝ} (hR : ‖CStarMatrix.ofMatrix a.matrix‖ ≤ R) : d.spectralValue a = ∫ t in (0 : ℝ)..R, d.distribution a t := by have he : (∫ t in ‖CStarMatrix.ofMatrix a.matrix‖..R, d.distribution a t) = 0 := by have h := intervalIntegral.integral_congr_Ioo_of_le (μ := volume) hR (g := fun _ : ℝ => (0 : ℝ)) (fun t ht => d.distribution_eq_zero a ht.1.le) simpa using h have h := intervalIntegral.integral_add_adjacent_intervals (d.distribution_intervalIntegrable a 0 ‖CStarMatrix.ofMatrix a.matrix‖) (d.distribution_intervalIntegrable a ‖CStarMatrix.ofMatrix a.matrix‖ R) rw [he, add_zero] at h exact h /-- Block addition is preserved by the finite spectral integral. -/ theorem spectralValue_add (d : CuntzDimensionState A) (a b : CuntzPositiveMatrix A) : d.spectralValue (a.add b) = d.spectralValue a + d.spectralValue b := by let R := ‖CStarMatrix.ofMatrix (a.add b).matrix‖ + ‖CStarMatrix.ofMatrix a.matrix‖ + ‖CStarMatrix.ofMatrix b.matrix‖ have ha : ‖CStarMatrix.ofMatrix a.matrix‖ ≤ R := by dsimp [R] linarith [norm_nonneg (CStarMatrix.ofMatrix (a.add b).matrix), norm_nonneg (CStarMatrix.ofMatrix a.matrix), norm_nonneg (CStarMatrix.ofMatrix b.matrix)] have hb : ‖CStarMatrix.ofMatrix b.matrix‖ ≤ R := by dsimp [R] linarith [norm_nonneg (CStarMatrix.ofMatrix (a.add b).matrix), norm_nonneg (CStarMatrix.ofMatrix a.matrix), norm_nonneg (CStarMatrix.ofMatrix b.matrix)] have hab : ‖CStarMatrix.ofMatrix (a.add b).matrix‖ ≤ R := by dsimp [R] linarith [norm_nonneg (CStarMatrix.ofMatrix (a.add b).matrix), norm_nonneg (CStarMatrix.ofMatrix a.matrix), norm_nonneg (CStarMatrix.ofMatrix b.matrix)] rw [d.spectralValue_eq_integral _ hab, d.spectralValue_eq_integral _ ha, d.spectralValue_eq_integral _ hb] simp_rw [d.distribution_add] exact intervalIntegral.integral_add (d.distribution_intervalIntegrable a 0 R) (d.distribution_intervalIntegrable b 0 R) /-- A normalized dimension state forces the underlying algebra to be nonzero. -/ theorem nontrivial (d : CuntzDimensionState A) : Nontrivial A := by rcases subsingleton_or_nontrivial A with h | h · let := h have he := d.regularized_of_matrix_eq_zero (.unit 1) (Subsingleton.elim _ _) rw [d.regularized_unit] at he norm_num at he · exact h theorem distribution_unit_of_lt (d : CuntzDimensionState A) (n : ℕ) {t : ℝ} (ht : t < 1) : d.distribution (.unit n) t = (n : ℝ) := by have hp : 0 < 1-t := sub_pos.mpr ht have he := cuntzCutoff_one_of_lt (A := CStarMatrix (Fin n) (Fin n) A) ht rw [← d.regularized_unit n] apply d.regularized_eq change CuntzEquivalent (CStarMatrix.ofMatrix.symm (cuntzCutoff (1 : CStarMatrix (Fin n) (Fin n) A) t)) (1 : Matrix (Fin n) (Fin n) A) rw [he] exact cuntzEquivalent_pos_smul 1 hp /-- The finite spectral integral has exactly the required matrix-unit values. -/ theorem spectralValue_unit (d : CuntzDimensionState A) (n : ℕ) : d.spectralValue (.unit n) = (n : ℝ) := by by_cases hn : n = 0 · subst n have h := d.spectralValue_le_norm_mul_size (.unit 0) have hp := d.spectralValue_nonneg (.unit 0) change d.spectralValue (.unit 0) ≤ ‖CStarMatrix.ofMatrix (CuntzPositiveMatrix.unit (A := A) 0).matrix‖ * ((0 : ℕ) : ℝ) at h rw [Nat.cast_zero, mul_zero] at h simpa only [Nat.cast_zero] using le_antisymm h hp · let := d.nontrivial let : Nonempty (Fin n) := Fin.pos_iff_nonempty.mp (Nat.pos_of_ne_zero hn) change (∫ t in (0 : ℝ)..‖(1 : CStarMatrix (Fin n) (Fin n) A)‖, d.distribution (.unit n) t) = _ rw [norm_one] have he := intervalIntegral.integral_congr_Ioo_of_le (μ := volume) (by norm_num : (0 : ℝ) ≤ 1) (f := d.distribution (.unit n)) (g := fun _ : ℝ => (n : ℝ)) (fun t ht => d.distribution_unit_of_lt n ht.2) simpa using he end CuntzDimensionState /-- Scaling the element rescales the spectral threshold. -/ theorem cuntzCutoff_pos_smul {a : A} (ha : 0 ≤ a) {r : ℝ} (hr : 0 < r) (t : ℝ) : cuntzCutoff (r • a) t = r • cuntzCutoff a (t/r) := by unfold cuntzCutoff rw [← cfc_comp_const_mul r (fun s : ℝ => max (s-t) 0) a (ha := ha.isSelfAdjoint), ← cfc_const_mul r (fun s : ℝ => max (s-t/r) 0) a] apply cfc_congr intro s hs dsimp only rw [mul_max_of_nonneg _ _ hr.le, mul_zero, mul_sub, mul_div_cancel₀ _ hr.ne'] /-- Nonnegative scalar multiplication of a positive finite matrix. -/ def CuntzPositiveMatrix.scale (a : CuntzPositiveMatrix A) (r : ℝ) (hr : 0 ≤ r) : CuntzPositiveMatrix A := ⟨a.size, CStarMatrix.ofMatrix.symm (r • CStarMatrix.ofMatrix a.matrix), smul_nonneg hr a.nonneg⟩ namespace CuntzDimensionState theorem distribution_pos_scale (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) {r : ℝ} (hr : 0 < r) (t : ℝ) : d.distribution (a.scale r hr.le) t = d.distribution a (t/r) := by apply d.regularized_eq have he := cuntzCutoff_pos_smul a.nonneg hr t have hc := cuntzEquivalent_pos_smul (cuntzCutoff (CStarMatrix.ofMatrix a.matrix) (t / r)) hr exact Eq.mpr (congrArg (fun c => CuntzEquivalent (CStarMatrix.ofMatrix.symm c) (CStarMatrix.ofMatrix.symm (cuntzCutoff (CStarMatrix.ofMatrix a.matrix) (t / r)))) he) hc /-- The integral scales with the positive scalar, including zero. -/ theorem spectralValue_scale (d : CuntzDimensionState A) (a : CuntzPositiveMatrix A) (r : ℝ) (hr : 0 ≤ r) : d.spectralValue (a.scale r hr) = r * d.spectralValue a := by rcases eq_or_lt_of_le hr with h | h · subst r have hn : ‖CStarMatrix.ofMatrix (a.scale 0 hr).matrix‖ = 0 := by change ‖(0 : ℝ) • CStarMatrix.ofMatrix a.matrix‖ = 0 rw [zero_smul, norm_zero] simp only [spectralValue, hn, intervalIntegral.integral_same, zero_mul] · let : NormedSpace ℝ (CStarMatrix (Fin a.size) (Fin a.size) A) := NormedSpace.restrictScalars ℝ ℂ _ let : NormSMulClass ℝ (CStarMatrix (Fin a.size) (Fin a.size) A) := NormedSpace.toNormSMulClass change (∫ t in (0 : ℝ)..‖r • CStarMatrix.ofMatrix a.matrix‖, d.distribution (a.scale r hr) t) = _ simp_rw [d.distribution_pos_scale a h] rw [norm_smul, Real.norm_of_nonneg hr, intervalIntegral.integral_comp_div _ h.ne'] simp only [zero_div, mul_div_cancel_left₀ _ h.ne', smul_eq_mul, spectralValue] end CuntzDimensionState end Kaplansky end end OAI