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MIPRE.Background.Repetition.CommutingRepetition.VN.Cyclic

The cyclic subspace #

The linear span of {x ξ | x ∈ S}.

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    The closed cyclic subspace [S ξ].

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      theorem CommutingRepetition.VN.apply_mem_orbit {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] {S : Set (H →L[ℂ] H)} {ξ : H} {x : H →L[ℂ] H} (hx : x ∈ S) :
      x ξ ∈ orbit S ξ
      theorem CommutingRepetition.VN.apply_mem_orbit_of_mem {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] (N : VonNeumannAlgebra H) (ξ : H) {x : H →L[ℂ] H} (hx : x ∈ N) {v : H} (hv : v ∈ orbit (↑N) ξ) :
      x v ∈ orbit (↑N) ξ

      The orbit of a von Neumann algebra is invariant under the algebra.

      theorem CommutingRepetition.VN.apply_mem_cyclicSpace_of_mem {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] (N : VonNeumannAlgebra H) (ξ : H) {x : H →L[ℂ] H} (hx : x ∈ N) {v : H} (hv : v ∈ cyclicSpace (↑N) ξ) :
      x v ∈ cyclicSpace (↑N) ξ

      The cyclic subspace of a von Neumann algebra is invariant under the algebra.

      The projection onto the cyclic subspace [N ξ].

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        The projection onto [N ξ] lies in the commutant N′.

        The projection onto [N′ ξ] lies in N.

        Cyclic and separating vectors #

        ξ is cyclic for S: span (S ξ) is dense.

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          ξ is separating for S: x ξ = 0 ⇒ x = 0 for x ∈ S.

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            A vector separating for N is cyclic for N′ ([N′ ξ]^⊥ is N-invariant, so its projection is in N and kills ξ).

            A vector cyclic for N′ is separating for N.

            theorem CommutingRepetition.VN.IsSeparating.mono {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] {S T : Set (H →L[ℂ] H)} {ξ : H} (h : IsSeparating T ξ) (hST : S ⊆ T) :
            theorem CommutingRepetition.VN.isSeparating_of_faithful {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] {S : Set (H →L[ℂ] H)} {ξ : H} (h : ∀ x ∈ S, inner ℂ ξ ((star x * x) ξ) = 0 → x = 0) :

            A vector state faithful on N gives a separating vector.

            From convergence at a separating vector to strong convergence #

            theorem CommutingRepetition.VN.tendsto_of_dense {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] {ι : Type u_2} {l : Filter ι} {T : ι → H →L[ℂ] H} {L : H →L[ℂ] H} {C : ℝ} (hC : ∀ (i : ι), ‖T i‖ ≤ C) {s : Set H} (hs : Dense s) (h : ∀ v ∈ s, Filter.Tendsto (fun (i : ι) => (T i) v) l (nhds (L v))) (ξ : H) :
            Filter.Tendsto (fun (i : ι) => (T i) ξ) l (nhds (L ξ))

            Bounded pointwise convergence on a dense set gives pointwise convergence everywhere.

            theorem CommutingRepetition.VN.tendstoStrongBdd_of_tendsto_separating {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] (N : VonNeumannAlgebra H) {ξ : H} (hξ : IsSeparating (↑N) ξ) {ι : Type u_2} {l : Filter ι} {T : ι → H →L[ℂ] H} {L : H →L[ℂ] H} (hT : ∀ (i : ι), T i ∈ N) (hL : L ∈ N) {C : ℝ} (hC : ∀ (i : ι), ‖T i‖ ≤ C) (h : Filter.Tendsto (fun (i : ι) => (T i) ξ) l (nhds (L ξ))) :

            Convergence at a separating vector, with a uniform norm bound, upgrades to bounded strong convergence (the commutant orbit N′ ξ is dense and T i (y ξ) = y (T i ξ)).