Documentation

MIPRE.Background.Repetition.CommutingRepetition.VN.Modular.PolarJ

Intertwining the continuous functional calculus #

theorem CommutingRepetition.VN.Modular.pow_intertwine {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] {A : K →L[] K} {S S' : K →L[] K} (h : ∀ (x : K), A (S x) = S' (A x)) (n : ) (x : K) :
A ((S ^ n) x) = (S' ^ n) (A x)
theorem CommutingRepetition.VN.Modular.aeval_intertwine {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] {A : K →L[] K} {S S' : K →L[] K} (h : ∀ (x : K), A (S x) = S' (A x)) (p : Polynomial ) (x : K) :
A (((Polynomial.aeval S) p) x) = ((Polynomial.aeval S') p) (A x)
theorem CommutingRepetition.VN.Modular.cfc_intertwine {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] {A : K →L[] K} {S S' : K →L[] K} (hS : IsSelfAdjoint S) (hS' : IsSelfAdjoint S') (h : ∀ (x : K), A (S x) = S' (A x)) {f : } (hf : Continuous f) (x : K) :
A ((cfc f S) x) = (cfc f S') (A x)

A real-linear operator intertwining two self-adjoint operators intertwines their continuous functional calculi (Weierstrass approximation).

T = |P − Q| = (R(2−R))^{1/2} and A = P − Q #

noncomputable def CommutingRepetition.VN.Modular.gT (l : ) :

√(λ(2−λ)), bounded by 1.

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    T := (R(2−R))^{1/2} (RvD's T, the modulus of P − Q).

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      theorem CommutingRepetition.VN.Modular.cfc_two_sub {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) :
      cfc (fun (l : ) => 2 - l) (R M Ω) = 2 - R M Ω
      theorem CommutingRepetition.VN.Modular.Tm_mul_Tm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) :
      Tm M Ω * Tm M Ω = R M Ω * (2 - R M Ω)

      T² = R(2−R) (RvD Prop. 2.2(2)).

      theorem CommutingRepetition.VN.Modular.Tm_eq_zero_iff {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) {x : K} :
      (Tm M Ω) x = 0 x = 0
      theorem CommutingRepetition.VN.Modular.Am_apply {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω x : K) :
      (Am M Ω) x = (Pre M Ω) x - (Qre M Ω) x
      theorem CommutingRepetition.VN.Modular.Am_Am {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω x : K) :
      (Am M Ω) ((Am M Ω) x) = (R M Ω * (2 - R M Ω)) x

      A² = R(2−R) (RvD Prop. 2.2(2)).

      theorem CommutingRepetition.VN.Modular.Am_R {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω x : K) :
      (Am M Ω) ((R M Ω) x) = (2 - R M Ω) ((Am M Ω) x)

      A R = (2 − R) A (RvD Prop. 2.2(5) via the polar decomposition).

      theorem CommutingRepetition.VN.Modular.Am_Tm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω x : K) :
      (Am M Ω) ((Tm M Ω) x) = (Tm M Ω) ((Am M Ω) x)

      A T = T A (RvD Prop. 2.2(4)).

      The antiunitary J: J (T x) = A x #

      @[reducible, inline]

      The range of T as a (dense) subspace.

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        theorem CommutingRepetition.VN.Modular.exists_rep_Tm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (v : (TmRange M Ω)) :
        ∃ (x : K), (Tm M Ω) x = v
        noncomputable def CommutingRepetition.VN.Modular.repT {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (v : (TmRange M Ω)) :
        K

        A preimage under T.

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          theorem CommutingRepetition.VN.Modular.Tm_repT {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (v : (TmRange M Ω)) :
          (Tm M Ω) (repT M Ω v) = v
          theorem CommutingRepetition.VN.Modular.repT_Tm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (x : K) :
          repT M Ω (Tm M Ω) x, = x
          theorem CommutingRepetition.VN.Modular.Am_eq_of_Tm_eq {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) {x y : K} (h : (Tm M Ω) x = (Tm M Ω) y) :
          (Am M Ω) x = (Am M Ω) y

          J₀ : T x ↦ A x on the range of T, conjugate-linear and isometric.

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          • One or more equations did not get rendered due to their size.
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            theorem CommutingRepetition.VN.Modular.J₀_apply {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (v : (TmRange M Ω)) :
            (J₀ M Ω) v = (Am M Ω) (repT M Ω v)

            The antiunitary J, the continuous extension of T x ↦ A x (RvD §2, the partial isometry of the polar decomposition P − Q = JT).

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              theorem CommutingRepetition.VN.Modular.Jm_Tm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (x : K) :
              (Jm M Ω) ((Tm M Ω) x) = (Am M Ω) x
              theorem CommutingRepetition.VN.Modular.Jm_smul {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (c : ) (ξ : K) :
              (Jm M Ω) (c ξ) = (starRingEnd ) c (Jm M Ω) ξ
              theorem CommutingRepetition.VN.Modular.ext_of_Tm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) {Y : Type u_2} [TopologicalSpace Y] [T2Space Y] {f g : KY} (hf : Continuous f) (hg : Continuous g) (h : ∀ (x : K), f ((Tm M Ω) x) = g ((Tm M Ω) x)) :
              f = g

              Two continuous maps agreeing on the range of T agree everywhere.

              theorem CommutingRepetition.VN.Modular.norm_Jm_apply {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ : K) :
              (Jm M Ω) ξ = ξ
              theorem CommutingRepetition.VN.Modular.Tm_Jm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ : K) :
              (Tm M Ω) ((Jm M Ω) ξ) = (Am M Ω) ξ

              T J = A (J commutes with T, RvD Prop. 2.2(4)).

              theorem CommutingRepetition.VN.Modular.Jm_Tm_comm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ : K) :
              (Jm M Ω) ((Tm M Ω) ξ) = (Tm M Ω) ((Jm M Ω) ξ)
              theorem CommutingRepetition.VN.Modular.inner_Jm_left_real {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ η : K) :
              inner ((Jm M Ω) ξ) η = inner ξ ((Jm M Ω) η)

              Real symmetry Re⟪Jξ, η⟫ = Re⟪ξ, Jη⟫.

              theorem CommutingRepetition.VN.Modular.inner_Jm_left {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ η : K) :
              inner ((Jm M Ω) ξ) η = inner ((Jm M Ω) η) ξ

              ⟪Jξ, η⟫ = ⟪Jη, ξ⟫ (RvD Prop. 3.1).

              theorem CommutingRepetition.VN.Modular.inner_Jm_Jm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ η : K) :
              inner ((Jm M Ω) ξ) ((Jm M Ω) η) = inner ξ η
              theorem CommutingRepetition.VN.Modular.Jm_Jm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ : K) :
              (Jm M Ω) ((Jm M Ω) ξ) = ξ

              J² = 1 (RvD Prop. 2.2(3)).

              theorem CommutingRepetition.VN.Modular.Jm_Ω {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) :
              (Jm M Ω) Ω = Ω
              theorem CommutingRepetition.VN.Modular.Jm_R {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ : K) :
              (Jm M Ω) ((R M Ω) ξ) = (2 - R M Ω) ((Jm M Ω) ξ)

              J R = (2 − R) J (RvD Prop. 2.2(5)).

              J and the functional calculus of R #

              J R = (2 − R) J transports the spectral data of R under λ ↦ 2 − λ: J g(R) = g(2 − R) J for every bounded Borel g.

              J as a real-linear operator.

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                theorem CommutingRepetition.VN.Modular.Jm_cfc {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) {f : } (hf : Continuous f) (x : K) :
                (Jm M Ω) ((cfc f (R M Ω)) x) = (cfc (fun (l : ) => f (2 - l)) (R M Ω)) ((Jm M Ω) x)

                J f(R) = f(2 − R) J = (f ∘ (2 − ·))(R) J for continuous f.

                theorem CommutingRepetition.VN.Modular.ν_Jm {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (ξ : K) :
                BorelCalc.ν (R M Ω) ((Jm M Ω) ξ) = MeasureTheory.Measure.map (fun (l : ) => 2 - l) (BorelCalc.ν (R M Ω) ξ)

                The spectral measure of R at J ξ is the push-forward of the one at ξ under λ ↦ 2 − λ.

                theorem CommutingRepetition.BorelCalc.Bdd.comp_two_sub {g : } (hg : Bdd g) :
                Bdd fun (l : ) => g (2 - l)

                Conjugation G ↦ J G J by the antiunitary J, a (complex-linear) operator.

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                  theorem CommutingRepetition.VN.Modular.conjJm_apply {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (G : K →L[] K) (ξ : K) :
                  (conjJm M Ω G) ξ = (Jm M Ω) (G ((Jm M Ω) ξ))
                  theorem CommutingRepetition.VN.Modular.Jm_bfc {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (g : ) (ξ : K) :
                  (Jm M Ω) ((BorelCalc.bfc (R M Ω) g) ξ) = (BorelCalc.bfc (R M Ω) fun (l : ) => g (2 - l)) ((Jm M Ω) ξ)

                  J g(R) = (g ∘ (2 − ·))(R) J for bounded Borel g.

                  theorem CommutingRepetition.VN.Modular.Jm_cbfc {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) {G : } (hG : BorelCalc.CBdd G) (ξ : K) :
                  (Jm M Ω) ((BorelCalc.cbfc (R M Ω) G) ξ) = (BorelCalc.cbfc (R M Ω) fun (l : ) => (starRingEnd ) (G (2 - l))) ((Jm M Ω) ξ)

                  θ(2 − l) = −θ l.

                  theorem CommutingRepetition.VN.Modular.Jm_Δit {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (t : ) (ξ : K) :
                  (Jm M Ω) ((Δit M Ω t) ξ) = (Δit M Ω t) ((Jm M Ω) ξ)

                  J Δ^{it} = Δ^{it} J (RvD Prop. 3.3).

                  theorem CommutingRepetition.VN.Modular.Δit_Kre {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) (t : ) {x : K} (hx : x Kre M Ω) :
                  (Δit M Ω t) x Kre M Ω

                  Δ^{it} preserves 𝒦 (RvD Prop. 3.3): P = (R + A)/2 commutes with Δ^{it}.

                  The bounded identities T J (x Ω) = (2 − R)(x* Ω), T J (x' Ω) = R (x'* Ω) (RvD Lemma 4.5) #

                  theorem CommutingRepetition.VN.Modular.Qre_commutant_sa {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) {a' : K →L[] K} (ha' : a' M.commutant) (hsa' : IsSelfAdjoint a') :
                  (Qre M Ω) (a' Ω) = 0

                  For self-adjoint a' ∈ M', Q (a' Ω) = 0: a' Ω ⊥ i𝒦.

                  theorem CommutingRepetition.VN.Modular.Am_sa_mem {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) {a : K →L[] K} (ha : a M) (hsa : IsSelfAdjoint a) :
                  (Am M Ω) (a Ω) = (2 - R M Ω) (a Ω)

                  For self-adjoint a ∈ M, T J (a Ω) = (2 − R)(a Ω).

                  theorem CommutingRepetition.VN.Modular.Am_commutant_sa {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) {a' : K →L[] K} (ha' : a' M.commutant) (hsa' : IsSelfAdjoint a') :
                  (Am M Ω) (a' Ω) = (R M Ω) (a' Ω)

                  For self-adjoint a' ∈ M', A (a' Ω) = R (a' Ω).

                  Conjugate-linearity of A in the form used for the decomposition x = a + i b.

                  theorem CommutingRepetition.VN.Modular.Tm_Jm_apply_mem {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) {x : K →L[] K} (hx : x M) :
                  (Tm M Ω) ((Jm M Ω) (x Ω)) = (2 - R M Ω) ((star x) Ω)

                  RvD Lemma 4.5 (first identity): T J (x Ω) = (2 − R)(x* Ω) for x ∈ M.

                  theorem CommutingRepetition.VN.Modular.Tm_Jm_apply_mem_commutant {K : Type u_1} [NormedAddCommGroup K] [InnerProductSpace K] [CompleteSpace K] (M : VonNeumannAlgebra K) (Ω : K) (hs : IsSeparating (↑M) Ω) (hc : IsCyclic (↑M) Ω) {x' : K →L[] K} (hx' : x' M.commutant) :
                  (Tm M Ω) ((Jm M Ω) (x' Ω)) = (R M Ω) ((star x') Ω)

                  RvD Lemma 4.5 (second identity): T J (x' Ω) = R (x'* Ω) for x' ∈ M'.