Abstract
The “twisted convolution” associated with the Weyl form of the canonical commutation relations forn degrees of freedom is decribed using ordinary convolution on a nilpotent central extension of additive phase space by the one-dimensional torus. Twisted convolution determines severalC*-algebras of quantum mechanical observables amongst which we study especially the algebra ℒ2(\(\mathfrak{E}\), σ) consisting of the ℒ2-functions on phase space and mapped isometrically onto the Hilbert-Schmidt-operators by the Schrödinger representation. The two last sections of the paper deal with “phase space quantum mechanics” from the point of view of twisted convolution: theWigner-Moyal formalism and the entire function formalism ofBargmann andSegal.
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Loupias, G., Miracle-Sole, S. C*-Algèbres des systèmes canoniques. I. Commun.Math. Phys. 2, 31–48 (1966). https://doi.org/10.1007/BF01773339
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DOI: https://doi.org/10.1007/BF01773339