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TauCeti.Analysis.CStarAlgebra.Action.Analytic

Entire analytic elements of C⋆-algebra actions #

For a point-norm continuous real action α on a possibly nonunital C⋆-algebra A, an element a is entire analytic when its orbit t ↦ α_t a is the restriction to the real line of an entire A-valued function. That function is unique, and α.entireExtension a z is its value α_z a at complex time z.

The entire analytic elements form a nonunital star subalgebra, on which the complex-time extension is complex linear, multiplicative and satisfies α_z (a⋆) = (α_{conj z} a)⋆. It is invariant under the action and its complex-time extension: α_w (α_z a) = α_{z + w} a. The norm of α_z a depends only on the imaginary part of z, so the extension is bounded on every horizontal strip of bounded width. An eigenvector α_t a = exp (c t) • a is entire analytic, with α_z a = exp (c z) • a. Entire analytic elements lie in the domain of the generator δ of α, where δ a is the complex derivative of the extension at 0, and the subalgebra is invariant under δ.

A continuous linear functional invariant under the action is also invariant in complex time on entire analytic elements, apply_entireExtension_of_apply_action, so its correlations satisfy φ (α_z(a) α_w(b)) = φ (a α_{w - z}(b)). For an invariant positive functional ω, the imaginary-time correlation ω (a⋆ α_{is}(a)) of an entire analytic a is nonnegative, apply_star_mul_entireExtension_mul_I_nonneg_of_apply_action.

These are the elements on which the analytic form ω(a α_{iβ}(b)) = ω(b a) of the KMS condition is stated.

References #

Bratteli--Robinson, Operator Algebras and Quantum Statistical Mechanics 1, second edition, Section 2.5.3, for entire analytic elements of one-parameter groups of automorphisms.

An element is entire analytic for a real action when its orbit t ↦ α_t a is the restriction to the real line of an entire A-valued function.

Instances For
    noncomputable def TauCeti.CStarAction.entireExtension {A : Type u_1} [NonUnitalCStarAlgebra A] (α : CStarAction (Multiplicative ℝ) A) (a : A) :
    ℂ → A

    The complex-time action z ↦ α_z a on an entire analytic element a: the unique entire continuation of its orbit. It is identically zero when a is not entire analytic.

    Instances For
      @[simp]

      The complex-time extension vanishes away from the entire analytic elements.

      The complex-time extension of an entire analytic element is entire.

      @[simp]

      At real times the complex-time extension is the action.

      @[simp]

      At time zero the complex-time extension is the identity.

      For an entire analytic b, the correlation function z ↦ φ (a α_z(b)) is entire.

      theorem TauCeti.CStarAction.entireExtension_eq_of_differentiable {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {a : A} {F : ℂ → A} (hF : Differentiable ℂ F) (hFt : ∀ (t : ℝ), F ↑t = (α (Multiplicative.ofAdd t)) a) :

      Uniqueness of continuation. Any entire extension of the orbit of a is the complex-time extension of a.

      An element is entire analytic exactly when its complex-time extension is an entire extension of its orbit.

      An eigenvector of the action, α_t a = exp (c t) • a, is entire analytic.

      theorem TauCeti.CStarAction.entireExtension_eq_exp_smul {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {a : A} {c : ℂ} (h : ∀ (t : ℝ), (α (Multiplicative.ofAdd t)) a = Complex.exp (c * ↑t) • a) (z : ℂ) :

      The complex-time extension of an eigenvector α_t a = exp (c t) • a is α_z a = exp (c z) • a.

      Time shift. Translating complex time by a real time t is the action of t.

      The values of the complex-time extension are again entire analytic.

      Group law in complex time. α_w (α_z a) = α_{z + w} a.

      The action at a real time preserves entire analyticity.

      The complex-time extension of a real translate is the translated extension.

      The norm of α_z a depends only on the imaginary part of z.

      Strip bound. The complex-time extension is bounded on every horizontal strip whose imaginary parts form a bounded set.

      @[simp]

      An element is entire analytic exactly when one of its real translates is.

      Algebraic operations #

      @[simp]

      The complex-time extension of zero vanishes.

      Sums of entire analytic elements are entire analytic.

      @[simp]

      The complex-time extension is additive.

      Scalar multiples of entire analytic elements are entire analytic.

      @[simp]

      The complex-time extension is complex linear.

      Negatives of entire analytic elements are entire analytic.

      @[simp]

      The complex-time extension commutes with negation.

      Differences of entire analytic elements are entire analytic.

      @[simp]

      The complex-time extension commutes with subtraction.

      Products of entire analytic elements are entire analytic.

      @[simp]

      The complex-time extension is multiplicative: α_z (a b) = α_z a α_z b.

      Adjoints of entire analytic elements are entire analytic.

      @[simp]

      Star relation. α_z (a⋆) = (α_{conj z} a)⋆.

      @[simp]

      Star preserves entire analyticity in both directions.

      The entire analytic elements of a real action, as a nonunital star subalgebra.

      Instances For
        @[simp]

        Membership in the entire analytic subalgebra is entire analyticity.

        The generator #

        Entire analytic elements lie in the domain of the generator.

        On an entire analytic element the generator is the complex derivative at time zero of the complex-time extension.

        The complex-time extension of the generator value is the derivative of the extension.

        The generator at a complex-time translate is the complex derivative of the extension there: δ(α_z(a)) = (d/dz) α_z(a).

        The generator maps entire analytic elements to entire analytic elements.

        The entire analytic subalgebra is contained in the generator domain.

        Invariant functionals #

        theorem TauCeti.CStarAction.apply_entireExtension_of_apply_action {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {b : A} {φ : A →L[ℂ] ℂ} (hφ : ∀ (t : Multiplicative ℝ) (a : A), φ ((α t) a) = φ a) (hb : α.IsEntireAnalytic b) (z : ℂ) :
        φ (α.entireExtension b z) = φ b

        Invariant functionals are invariant in complex time. If a continuous linear functional φ satisfies φ (α_t a) = φ a for all real t, then φ (α_z b) = φ b for every entire analytic b and every complex time z.

        theorem TauCeti.CStarAction.apply_entireExtension_mul_entireExtension_of_apply_action {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {a b : A} {φ : A →L[ℂ] ℂ} (hφ : ∀ (t : Multiplicative ℝ) (a : A), φ ((α t) a) = φ a) (ha : α.IsEntireAnalytic a) (hb : α.IsEntireAnalytic b) (z w : ℂ) :
        φ (α.entireExtension a z * α.entireExtension b w) = φ (a * α.entireExtension b (w - z))

        For an invariant continuous linear functional φ and entire analytic a, b, φ (α_z(a) α_w(b)) = φ (a α_{w - z}(b)).

        theorem TauCeti.CStarAction.apply_star_entireExtension_mul_entireExtension_of_apply_action {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {a : A} {φ : A →L[ℂ] ℂ} (hφ : ∀ (t : Multiplicative ℝ) (a : A), φ ((α t) a) = φ a) (ha : α.IsEntireAnalytic a) (z w : ℂ) :
        φ (star (α.entireExtension a z) * α.entireExtension a w) = φ (star a * α.entireExtension a (w - (starRingEnd ℂ) z))

        For an invariant continuous linear functional φ and an entire analytic a, φ ((α_z(a))⋆ α_w(a)) = φ (a⋆ α_{w - conj z}(a)).

        theorem TauCeti.CStarAction.apply_star_entireExtension_mul_I_mul_entireExtension_mul_I_of_apply_action {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {a : A} {φ : A →L[ℂ] ℂ} (hφ : ∀ (t : Multiplicative ℝ) (a : A), φ ((α t) a) = φ a) (ha : α.IsEntireAnalytic a) (s t : ℝ) :
        φ (star (α.entireExtension a (↑s * Complex.I)) * α.entireExtension a (↑t * Complex.I)) = φ (star a * α.entireExtension a (↑(s + t) * Complex.I))

        For an invariant continuous linear functional φ and an entire analytic a, imaginary-time correlations add: φ ((α_{is}(a))⋆ α_{it}(a)) = φ (a⋆ α_{i(s + t)}(a)) for real s, t.

        theorem TauCeti.CStarAction.apply_star_mul_entireExtension_mul_I_nonneg_of_apply_action {A : Type u_1} [NonUnitalCStarAlgebra A] {α : CStarAction (Multiplicative ℝ) A} {a : A} [PartialOrder A] [StarOrderedRing A] {ω : A →P[ℂ] ℂ} (hω : ∀ (t : Multiplicative ℝ) (a : A), ω ((α t) a) = ω a) (ha : α.IsEntireAnalytic a) (s : ℝ) :
        0 ≤ ω (star a * α.entireExtension a (↑s * Complex.I))

        For an invariant positive functional ω and an entire analytic a, the imaginary-time correlation ω (a⋆ α_{is}(a)) is nonnegative for every real s.

        Examples #

        @[simp]

        For the trivial action every element is entire analytic.

        @[simp]

        For the trivial action the complex-time extension is constant.

        @[simp]

        In a unital algebra the identity is entire analytic.

        @[simp]

        The complex-time extension of the identity is constant.