2016
DOI: 10.1016/j.geomphys.2015.09.013
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Strict deformation quantization of locally convex algebras and modules

Abstract: In this work various symbol spaces with values in a sequentially complete locally convex vector space are introduced and discussed. They are used to define vector-valued oscillatory integrals which allow to extend Rieffel's strict deformation quantization to the framework of sequentially complete locally convex algebras and modules with separately continuous products and module structures, making use of polynomially bounded actions of R n . Several well-known integral formulas for star products are shown to fi… Show more

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Cited by 20 publications
(28 citation statements)
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“…In particular, the task is to establish smoothness of the oscillatory integral in a suitable locally convex topology and to demonstrate that all derivatives are polynomially bounded (see [And13, Theorem 1] for a similar proof). After this is established, we build on results of [LW11] where smoothness and polynomial boundedness are the requirements needed in order to prove the well-definedness of the warped convolutions integral. Now for the spatial part a simpler route will be chosen.…”
Section: Qft-moyal-weyl From Deformationmentioning
confidence: 99%
“…In particular, the task is to establish smoothness of the oscillatory integral in a suitable locally convex topology and to demonstrate that all derivatives are polynomially bounded (see [And13, Theorem 1] for a similar proof). After this is established, we build on results of [LW11] where smoothness and polynomial boundedness are the requirements needed in order to prove the well-definedness of the warped convolutions integral. Now for the spatial part a simpler route will be chosen.…”
Section: Qft-moyal-weyl From Deformationmentioning
confidence: 99%
“…Note that Theorem 3.10 also shows that ω zb depends holomorphically on z ∈ in so far as ∋ z → ω zb (X) ∈ is holomorphic for all X ∈ S • (V ). This is the analog of statements in [12,13] in the Rieffel setting. Proposition 3.30 Let · be a continuous antilinear involution of V and Λ a continuous Hermitian bilinear forms on V .…”
Section: )mentioning
confidence: 75%
“…The former definition is rigorously defined for a certain bounded operators, see [BLS11]. However, since we are dealing with unbounded operators we use the results of [LW11] in order to prove that the deformation of the Coleman-Mandula operator is well-defined. Hence, let us consider the deformed operator A Θ as follows Definition 3.2.…”
Section: Mathematical Properties Of the Deformationmentioning
confidence: 99%