import Mathlib import OAI.Analysis.Commutator.AtomicCoefficients import OAI.Analysis.Commutator.AtomicDecomposition import OAI.Analysis.Commutator.MinimalCorner namespace OAI noncomputable section section noncomputable section open scoped ComplexOrder InnerProductSpace namespace Kadison.AtomicFactor.Decomposition variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} {p : H →L[ℂ] H} (D : Decomposition M p) theorem finite_dimensional [Finite D.I] (hp : IsMinimalProjection M p) : FiniteDimensional ℂ M := by classical let := Fintype.ofFinite D.I let K : Submodule ℂ (H →L[ℂ] H) := Submodule.span ℂ {p} have hcoeff (a : M) (ij : D.I×D.I) : star (D.v ij.1)*(a:H →L[ℂ] H)*D.v ij.2∈K := by have hpa : p*star (D.v ij.1)=star (D.v ij.1) := by simpa only [star_mul,hp.2.1.isSelfAdjoint.star_eq] using congrArg star (D.source ij.1) obtain ⟨z,hz⟩ := corner_scalar M hp (M.mul_mem (M.mul_mem (M.star_mem' (D.mem ij.1)) a.property) (D.mem ij.2)) (by rw [←mul_assoc,←mul_assoc,hpa]) (by rw [mul_assoc,D.source]) rw [hz] exact K.smul_mem z (Submodule.subset_span (Set.mem_singleton p)) let L : M →ₗ[ℂ] ((D.I×D.I) → K) := { toFun := fun a ij => ⟨star (D.v ij.1)*(a:H →L[ℂ] H)*D.v ij.2,hcoeff a ij⟩ map_add' := by intro a b funext ij apply Subtype.ext change star (D.v ij.1)*((a:H →L[ℂ] H)+(b:H →L[ℂ] H))*D.v ij.2= star (D.v ij.1)*(a:H →L[ℂ] H)*D.v ij.2+star (D.v ij.1)*(b:H →L[ℂ] H)*D.v ij.2 rw [mul_add,add_mul] map_smul' := by intro c a funext ij apply Subtype.ext change star (D.v ij.1)*(c • (a:H →L[ℂ] H))*D.v ij.2= c • (star (D.v ij.1)*(a:H →L[ℂ] H)*D.v ij.2) rw [mul_smul_comm,smul_mul_assoc] } apply FiniteDimensional.of_injective L intro a b hab apply Subtype.ext apply D.eq_of_coefficients_eq intro i j exact congrArg (fun f : (D.I×D.I) → K => ((f (i,j)):H →L[ℂ] H)) hab end Kadison.AtomicFactor.Decomposition end end end end OAI