import Mathlib import OAI.Analysis.Commutator.AtomicCoefficients namespace OAI noncomputable section section noncomputable section open scoped ComplexOrder InnerProductSpace Topology BigOperators open Filter 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) def finiteShift (f : D.I → D.I) (s : Finset D.I) : H →L[ℂ] H := ∑ i∈s,D.v (f i)*star (D.v i) lemma finiteShift_star_mul (f : D.I → D.I) (hf : Function.Injective f) (s : Finset D.I) : star (D.finiteShift f s)*D.finiteShift f s=D.support s := by classical rw [finiteShift,star_sum,Finset.sum_mul,support] apply Finset.sum_congr rfl intro i hi rw [Finset.mul_sum,Finset.sum_eq_single_of_mem i hi] · simp only [star_mul,star_star] calc _=(D.v i*(star (D.v (f i))*D.v (f i)))*star (D.v i) := by noncomm_ring _=D.v i*star (D.v i) := by rw [D.initial,D.source] · intro j hj hne simp only [star_mul,star_star] calc _=(D.v i*(star (D.v (f i))*D.v (f j)))*star (D.v j) := by noncomm_ring _=0 := by rw [D.cross (f i) (f j) (fun h => hne (hf h).symm),mul_zero,zero_mul] lemma finiteShift_norm_le (f : D.I → D.I) (hf : Function.Injective f) (s : Finset D.I) : ‖D.finiteShift f s‖≤1 := by have he := D.support_norm_le s rw [←D.finiteShift_star_mul f hf s,CStarRing.norm_star_mul_self] at he nlinarith [norm_nonneg (D.finiteShift f s)] lemma finiteShift_mul_val (f : D.I → D.I) (s : Finset D.I) {i : D.I} (hi : i∈s) : D.finiteShift f s*D.v i=D.v (f i) := by classical rw [finiteShift,Finset.sum_mul,Finset.sum_eq_single_of_mem i hi,mul_assoc,D.initial,D.source] intro j hj hne rw [mul_assoc,D.cross j i hne,mul_zero] theorem exists_shift (f : D.I → D.I) (hf : Function.Injective f) : ∃ W : H →L[ℂ] H,W∈M ∧ ∀ i,W*D.v i=D.v (f i) := by classical let ω : Ultrafilter (Finset D.I) := Ultrafilter.of atTop have hω : (ω : Filter (Finset D.I))≤atTop := Ultrafilter.of_le _ obtain ⟨W,hW,hlim⟩ := WeakOperatorLimit.exists_ultralimit ω (D.finiteShift f) 1 (by norm_num) (D.finiteShift_norm_le f hf) have hWM : W∈M := WeakOperatorLimit.mem_vonNeumann hlim M (Eventually.of_forall fun s => M.sum_mem (fun i _ => M.mul_mem (D.mem (f i)) (M.star_mem' (D.mem i)))) refine ⟨W,hWM,?_⟩ intro i ext x apply ext_inner_right ℂ intro y apply tendsto_nhds_unique (hlim (D.v i x) y) apply tendsto_const_nhds.congr' filter_upwards [hω (eventually_ge_atTop ({i}:Finset D.I))] with s hs have he := D.finiteShift_mul_val f s (i:=i) (hs (Finset.mem_singleton_self i)) exact congrArg (fun T : H →L[ℂ] H => inner ℂ (T x) y) he.symm lemma shift_isometry (f : D.I → D.I) (hf : Function.Injective f) {W : H →L[ℂ] H} (hW : ∀ i,W*D.v i=D.v (f i)) : star W*W=1 := by apply D.eq_of_coefficients_eq intro i j calc star (D.v i)*(star W*W)*D.v j=star (W*D.v i)*(W*D.v j) := by rw [star_mul]; noncomm_ring _=star (D.v (f i))*D.v (f j) := by rw [hW i,hW j] _=star (D.v i)*D.v j := by by_cases hij : i=j · subst j; rw [D.initial,D.initial] · rw [D.cross i j hij,D.cross (f i) (f j) (fun h => hij (hf h))] _=star (D.v i)*1*D.v j := by rw [mul_one] lemma shifts_orthogonal (f g : D.I → D.I) (hfg : ∀ i j,f i≠g j) {W V : H →L[ℂ] H} (hW : ∀ i,W*D.v i=D.v (f i)) (hV : ∀ i,V*D.v i=D.v (g i)) : star W*V=0 := by apply D.eq_zero_of_coefficients_zero intro i j calc _=star (W*D.v i)*(V*D.v j) := by rw [star_mul]; noncomm_ring _=star (D.v (f i))*D.v (g j) := by rw [hW i,hV j] _=0 := D.cross _ _ (hfg i j) end Kadison.AtomicFactor.Decomposition end end end end OAI