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TauCeti.Analysis.CStarAlgebra.Action.Covariant.Basic

Covariant representations of C⋆-actions #

A covariant representation consists of a possibly degenerate coefficient representation and a strongly continuous unitary group representation, satisfying U g (π a v) = π (α g a) (U g v). Strong continuity is imposed separately from ContRepresentation, which only makes each individual operator continuous. These data admit vector-valued integrated forms without assuming operator-norm continuity of the group representation.

The conventions follow Dana Williams, Crossed Products of C-Algebras*, Chapter 2.

structure TauCeti.CStarAction.CovariantRepresentation {G : Type u_1} {A : Type u_2} [Group G] [TopologicalSpace G] [NonUnitalCStarAlgebra A] (α : CStarAction G A) (H : Type u_4) [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] :
Type (max (max u_1 u_2) u_4)

A covariant pair for a point-norm continuous action on a possibly nonunital C⋆-algebra. The coefficient representation is not required to be nondegenerate.

  • coefficient : A →⋆ₙₐ[ℂ] H →L[ℂ] H

    The coefficient representation.

  • The group representation by bounded operators.

  • isUnitary : self.group.IsUnitary

    Each group operator preserves the inner product.

  • continuous_orbit (v : H) : Continuous fun (g : G) => (self.group g) v

    Every group orbit is continuous in the Hilbert-space norm.

  • covariance (g : G) (a : A) (v : H) : (self.group g) ((self.coefficient a) v) = (self.coefficient ((α g) a)) ((self.group g) v)

    Covariance of the coefficient and group representations.

Instances For

    The coefficient and group representations determine a covariant pair.

    @[simp]

    Covariance as an equality of bounded operators.

    The coefficient at a transformed element is obtained by unitary conjugation.

    Every coefficient representation gives a covariant pair for the trivial action, with trivial group representation.

    Instances For