2004
DOI: 10.1063/1.1757036
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Construction and uniqueness of the C*-Weyl algebra over a general pre-symplectic space

Abstract: A systematic approach to the C*-Weyl algebra W(E,σ) over a possibly degenerate pre-symplectic form σ on a real vector space E of possibly infinite dimension is elaborated in an almost self-contained manner. The construction is based on the theory of Kolmogorov decompositions for σ-positive-definite functions on involutive semigroups and their associated projective unitary group representations. The σ-positive-definite functions provide also the C*-norm of W(E,σ), the latter being shown to be *-isomorphic to th… Show more

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Cited by 33 publications
(54 citation statements)
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“…For the case of symplectic vector spaces the theory of CCR-representations is well understood and details can be found in [BGP07,BG12,BR96]. The generalization to presymplectic vector spaces has been studied in [BHR04] …”
Section: A Ccr-representations Of Generic Presymplectic Abelian Groupsmentioning
confidence: 99%
“…For the case of symplectic vector spaces the theory of CCR-representations is well understood and details can be found in [BGP07,BG12,BR96]. The generalization to presymplectic vector spaces has been studied in [BHR04] …”
Section: A Ccr-representations Of Generic Presymplectic Abelian Groupsmentioning
confidence: 99%
“…(For twisted group algebras we defer the reader to the citations in Subsection 3.2, and for the Weyl algebra with degenerate σ see [30,31], and references therein.) The C * -norm on W(E, σ) is denoted by · .…”
Section: Weyl Algebramentioning
confidence: 99%
“…In virtue of the linear independence of the W (f ), f ∈ E, β is a well-defined * -isomorphism from ∆(E, σ) onto ∆(E, σ). Extend norm-continuously using a result in [31].…”
Section: * -Isomorphisms For the Quantum Weyl Algebrasmentioning
confidence: 99%
“…Here T is an element of the group symp(E, σ) of all symplectic transformations on the pre-symplectic space (E, σ). (Recall that T ∈ symp(E, σ) is an R-linear bijection on E with σ(f, g) = σ(T f, T g); [24]). With Eq.…”
Section: Theorem 44 (Continuous and Strict Deformation Quantizationsmentioning
confidence: 99%
“…may be realized in terms of a bivector field, applied to differentials. For this we introduce an arbitrary locally convex Hausdorff vector space topology τ on E. On the topological dual space E τ of E we consider the σ(E τ , E)-topology, and so the bidual is given by (E τ ) = E. According to [24] the commutative C*-Weyl algebra W(E, 0) is *-isomorphic to the C*-algebra of the almost periodic, σ(E τ , E)-continuous functions on E τ , and we may regard each element A ∈ W(E, 0) as an almost periodic function A : E τ → C. The Weyl elements W 0 (f ) are realized in terms of the periodic functions (3.11)…”
mentioning
confidence: 99%