Joint continuity of x ↦ U x (ζ x) for uniformly bounded strongly continuous U #
The weak integral W = ∫ w_φ(t) Δ^{it} B Δ^{-it} dt #
Integrability of t ↦ w φ t • v t for bounded continuous v : ℝ → K.
The integrand t ↦ w φ t • Δ^{it} B Δ^{-it} ξ.
Equations
- CommutingRepetition.VN.Modular.Wint M Ω B φ ξ t = ↑(CommutingRepetition.StripCauchy.w φ t) • (CommutingRepetition.VN.Modular.Δit M Ω t) (B ((CommutingRepetition.VN.Modular.Δit M Ω (-t)) ξ))
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The operator W.
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- One or more equations did not get rendered due to their size.
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The bilinear form β(u, v) = ⟪J u, v⟫ #
β(u, v) = ⟪J u, v⟫, a continuous ℂ-bilinear form.
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- One or more equations did not get rendered due to their size.
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RvD Lemma 4.7 #
Δ^{it} commutes with 2 − R.
The function f(z) = ⟪η, E(z) x E(−z) ξ⟫.
Equations
- CommutingRepetition.VN.Modular.fz M Ω x η ξ z = inner ℂ η ((CommutingRepetition.VN.Modular.Efam M Ω z) (x ((CommutingRepetition.VN.Modular.Efam M Ω (-z)) ξ)))
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On the strip, f(z) = β(E(−z) Jη, x E(−z) ξ).
The operator identity behind λ f(1/2+it) + λ̄ f(-1/2+it) = ⟪η, T Δ^{it} B Δ^{-it} T ξ⟫.
RvD Lemma 4.7: T x T = T W T for x as in Lemma 4.5 (with λ = e^{iφ/2}).
RvD Lemma 4.7 (operator form): x = ∫ w_φ(t) Δ^{it} (J x′ J) Δ^{-it} dt.
For self-adjoint x′ ∈ M′ and |φ| < π, the weak integral W lies in M.
RvD Lemma 4.8: Δ^{it} (J x′ J) Δ^{-it} ∈ M #
Every x ∈ N is a + i b with a, b ∈ N self-adjoint.
RvD Lemma 4.8 (self-adjoint case): Δ^{it} (J x′ J) Δ^{-it} ∈ M for self-adjoint
x′ ∈ M′, by Laplace-transform uniqueness applied to the commutator with y′ ∈ M′.
RvD Lemma 4.8: Δ^{it} (J x′ J) Δ^{-it} ∈ M for every x′ ∈ M′.
J M′ J ⊆ M.
RvD Lemma 4.9: J M J ⊆ M′ #
For ξ ∈ 𝒦, Q (J ξ) = 0.
For ξ, η ∈ 𝒦, ⟪J ξ, η⟫ is real.
Claim A (self-adjoint case): ⟪Ω, y J x Ω⟫ = ⟪x J y Ω, Ω⟫ for x, y ∈ M_s.
Claim A: ⟪Ω, y J x Ω⟫ = ⟪x J y Ω, Ω⟫ for x, y ∈ M.
Claim B: (J y J)(x Ω) = x (J y J Ω) for x, y ∈ M.
RvD Lemma 4.9: J M J ⊆ M′.
RvD Theorem 4.2 and the modular automorphism group #
Tomita's theorem, part 1: J M J = M′.
Tomita's theorem, part 1′: J M′ J = M.
The modular automorphism group σ_t(x) = Δ^{it} x Δ^{-it}.
Equations
- CommutingRepetition.VN.Modular.σ M Ω t x = CommutingRepetition.VN.Modular.Δit M Ω t * x * CommutingRepetition.VN.Modular.Δit M Ω (-t)
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Tomita's theorem, part 2: Δ^{it} M Δ^{-it} ⊆ M.
ψ ∘ σ_t = ψ for the vector state ψ = ⟪Ω, · Ω⟫.
Elements commuting with R are fixed by the modular group.