Operator-algebra dynamics, crossed products, and equilibrium
The declarations the status of Tau Ceti's roadmap names as Tau Ceti has them at commit ace60277.
TheoremDense analytic KMS criterion#
A state is β-KMS if and only if the analytic KMS identity holds for pairs in a norm-dense invariant set of entire analytic elements. In particular, the set can be a norm-dense invariant star subalgebra.
TauCeti.CStarAction.isKMSState_iff_of_dense.{u_1} {A : Type u_1} [NonUnitalCStarAlgebra A]
{α : TauCeti.CStarAction (Multiplicative ℝ) A} {β : ℝ} [PartialOrder A] [StarOrderedRing A]
{ω : A →P[ℂ] ℂ} {s : Set A} (hs : Dense s) (hinv : IsInvariant (fun t a => (α t) a) s)
(hentire : ∀ b ∈ s, α.IsEntireAnalytic b) :
α.IsKMSState β ω ↔
‖ω.toContinuousLinearMap‖ = 1 ∧
∀ a ∈ s, ∀ b ∈ s, ω (a * α.entireExtension b (↑β * Complex.I)) = ω (b * a)
Uses 1 · Used by 3
TheoremKMS states are invariant#
For β ≠ 0, every β-KMS state ω is invariant under the
dynamics: ω (α_t(a)) = ω a. At β = 0 the KMS states are the tracial states, which need not
be invariant.
TauCeti.CStarAction.IsKMSState.apply_action.{u_1} {A : Type u_1} [NonUnitalCStarAlgebra A]
{α : TauCeti.CStarAction (Multiplicative ℝ) A} {β : ℝ} [PartialOrder A] [StarOrderedRing A]
{ω : A →P[ℂ] ℂ} (hω : α.IsKMSState β ω) (hβ : β ≠ 0) (t : Multiplicative ℝ) (a : A) :
ω ((α t) a) = ω a
TheoremConvexity of K_β#
Convex combinations of β-KMS states are β-KMS states.
TauCeti.CStarAction.convex_kmsStates.{u_1} {A : Type u_1} [NonUnitalCStarAlgebra A] [PartialOrder A]
[StarOrderedRing A] {α : TauCeti.CStarAction (Multiplicative ℝ) A} {β : ℝ} :
Convex ℝ (α.kmsStates β)
TheoremWeak-* compactness of K_β#
For unital B, the set of β-KMS states is weak-* compact.
TauCeti.CStarAction.isCompact_kmsStates.{u_2} {B : Type u_2} [CStarAlgebra B] [PartialOrder B]
[StarOrderedRing B] {α : TauCeti.CStarAction (Multiplicative ℝ) B} {β : ℝ} :
IsCompact (α.kmsStates β)
TheoremPointwise limits of KMS states#
If β-KMS states converge pointwise to a positive functional of norm one, then the limit is a β-KMS state.
TauCeti.CStarAction.IsKMSState.of_tendsto.{u_1, u_2} {A : Type u_1} [NonUnitalCStarAlgebra A]
[PartialOrder A] [StarOrderedRing A] {α : TauCeti.CStarAction (Multiplicative ℝ) A} {β : ℝ}
{ω : A →P[ℂ] ℂ} {ι : Type u_2} {l : Filter ι} [l.NeBot] {ω' : ι → A →P[ℂ] ℂ}
(hω' : ∀ᶠ (i : ι) in l, α.IsKMSState β (ω' i))
(hlim : ∀ (a : A), Filter.Tendsto (fun i => (ω' i) a) l (nhds (ω a)))
(hnorm : ‖ω.toContinuousLinearMap‖ = 1) : α.IsKMSState β ω
TheoremTauCeti.CStarAction.CovariantRepresentation.integratedOperator_convolution#
The integrated form of a covariant pair is multiplicative for twisted convolution with respect
to a left-invariant measure: (π ⋊ U) (f ⋆ g) = (π ⋊ U) f * (π ⋊ U) g.
TauCeti.CStarAction.CovariantRepresentation.integratedOperator_convolution.{u_1, u_2, u_3}
{G : Type u_1} {A : Type u_2} {H : Type u_3} [Group G] [TopologicalSpace G] [MeasurableSpace G]
[OpensMeasurableSpace G] [NonUnitalCStarAlgebra A] [NormedAddCommGroup H] [InnerProductSpace ℂ H]
[CompleteSpace H] {α : TauCeti.CStarAction G A} (P : α.CovariantRepresentation H)
(μ : MeasureTheory.Measure G) [MeasureTheory.IsFiniteMeasureOnCompacts μ] [IsTopologicalGroup G]
[MeasurableMul G] [μ.IsMulLeftInvariant] (f g : CompactlySupportedContinuousMap G A) :
(P.integratedOperator μ) (((α.convolution μ) f) g) =
(P.integratedOperator μ) f * (P.integratedOperator μ) g
Lean
Formalized in Tau Ceti as TauCeti.CStarAction.CovariantRepresentation.integratedOperator_convolution.
Sources
- Tau Ceti documentation:
TauCeti.CStarAction.CovariantRepresentation.integratedOperator_convolution - Source of
TauCeti.CStarAction.CovariantRepresentation.integratedOperator_convolutionin TauCeti/Analysis/CStarAlgebra/Action/Covariant/Integrated.lean - Tau Ceti roadmap status: Operator-algebra dynamics, crossed products, and equilibrium
TheoremTauCeti.CStarAction.CovariantRepresentation.norm_integratedOperator_le#
The integrated form is bounded by the coefficient function's L¹ norm.
TauCeti.CStarAction.CovariantRepresentation.norm_integratedOperator_le.{u_1, u_2, u_3}
{G : Type u_1} {A : Type u_2} {H : Type u_3} [Group G] [TopologicalSpace G] [MeasurableSpace G]
[OpensMeasurableSpace G] [NonUnitalCStarAlgebra A] [NormedAddCommGroup H] [InnerProductSpace ℂ H]
[CompleteSpace H] {α : TauCeti.CStarAction G A} (P : α.CovariantRepresentation H)
(μ : MeasureTheory.Measure G) [MeasureTheory.IsFiniteMeasureOnCompacts μ]
(f : CompactlySupportedContinuousMap G A) : ‖(P.integratedOperator μ) f‖ ≤ ∫ (g : G), ‖f g‖ ∂μ
Lean
Formalized in Tau Ceti as TauCeti.CStarAction.CovariantRepresentation.norm_integratedOperator_le.
Sources
- Tau Ceti documentation:
TauCeti.CStarAction.CovariantRepresentation.norm_integratedOperator_le - Source of
TauCeti.CStarAction.CovariantRepresentation.norm_integratedOperator_lein TauCeti/Analysis/CStarAlgebra/Action/Covariant/Integrated.lean - Tau Ceti roadmap status: Operator-algebra dynamics, crossed products, and equilibrium
StructureTauCeti.CStarAction.ConvolutionAlgebra#
The convolution ⋆-algebra of the C⋆-dynamical system (A, G, α) with respect to μ: the
compactly supported continuous functions G → A, with twisted convolution as product and the
twisted involution as star. Use ConvolutionAlgebra.toConv and ConvolutionAlgebra.ofConv to
pass to and from C_c(G, A), whose own product and star are pointwise.
TauCeti.CStarAction.ConvolutionAlgebra.{u_1, u_2} {G : Type u_1} {A : Type u_2} [Group G]
[TopologicalSpace G] [NonUnitalCStarAlgebra A] [MeasurableSpace G] (α : TauCeti.CStarAction G A)
(μ : MeasureTheory.Measure G) : Type (max u_1 u_2)
DefinitionTauCeti.CStarAction.CovariantRepresentation.regular#
The regular covariant representation on L²(G, H) induced by a representation ρ of A on
H: a acts by ξ ↦ (r ↦ ρ (α_{r⁻¹}(a)) (ξ r)) and s by left translation
ξ ↦ (r ↦ ξ (s⁻¹ r)).
TauCeti.CStarAction.CovariantRepresentation.regular.{u_1, u_2, u_3} {G : Type u_1} {A : Type u_2}
{H : Type u_3} [Group G] [TopologicalSpace G] [NonUnitalCStarAlgebra A] [NormedAddCommGroup H]
[InnerProductSpace ℂ H] [CompleteSpace H] [IsTopologicalGroup G] [MeasurableSpace G]
[BorelSpace G] (α : TauCeti.CStarAction G A) (ρ : A →⋆ₙₐ[ℂ] H →L[ℂ] H)
(μ : MeasureTheory.Measure G) [μ.IsMulLeftInvariant] [μ.InnerRegularCompactLTTop]
[MeasureTheory.IsLocallyFiniteMeasure μ] : α.CovariantRepresentation ↥(MeasureTheory.Lp H 2 μ)
Lean
Formalized in Tau Ceti as TauCeti.CStarAction.CovariantRepresentation.regular.
Sources
DefinitionTauCeti.CStarAction.entireAnalytic#
The entire analytic elements of a real action, as a nonunital star subalgebra.
TauCeti.CStarAction.entireAnalytic.{u_1} {A : Type u_1} [NonUnitalCStarAlgebra A]
(α : TauCeti.CStarAction (Multiplicative ℝ) A) : NonUnitalStarSubalgebra ℂ A
TheoremDensity of entire analytic elements#
The entire analytic elements of a point-norm continuous real action are dense, since every element is a limit of its Gaussian smearings.
TauCeti.CStarAction.dense_entireAnalytic.{u_1} {A : Type u_1} [NonUnitalCStarAlgebra A]
(α : TauCeti.CStarAction (Multiplicative ℝ) A) : Dense ↑α.entireAnalytic
Uses 1 · Used by 4
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