1966
DOI: 10.1007/bf01773339
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C*-Algèbres des systèmes canoniques. I

Abstract: The "twisted convolution" associated with the Weyl form of the canonical commutation relations for n degrees of freedom is decribed using ordinary convolution on a nilpotent central extension of additive phase space by the onedimensional torus. Twisted convolution determines several O*-algebras of quantum mechanical observables amongst which we study especially the algebra £f 2 (&> o) consisting of the oδf 2 -functions on phase space and mapped isometrically onto the Hilbert-Schmidt-operators by the Schrόdinge… Show more

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Cited by 77 publications
(58 citation statements)
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“…must be positive semidefinite, which becomes the necessary condition forρ q to be positive semidefinite. According to KLM [14,15], the converse is also true, i.e., the positive semidefiniteness of all matrices {M ij } becomes sufficient for that ofρ q . In our heuristic argument, this sufficiency may be seen, with less mathematical rigor, as follows.…”
Section: Klm Conditionsmentioning
confidence: 99%
“…must be positive semidefinite, which becomes the necessary condition forρ q to be positive semidefinite. According to KLM [14,15], the converse is also true, i.e., the positive semidefiniteness of all matrices {M ij } becomes sufficient for that ofρ q . In our heuristic argument, this sufficiency may be seen, with less mathematical rigor, as follows.…”
Section: Klm Conditionsmentioning
confidence: 99%
“…By the parametrix formula in the scalar case, to the above q, there correspond a positive integer r, an element gEC co (W) 9 and an element heC q (W) such that Remark. One may find a prototype of the above theorem in G. Loupias and S. Miracle-Sole's paper [5], which tells us that any operator of the Schrodinger representation can be considered as a tempered distribution on the phase space of a system with n degrees of freedom.…”
Section: = Fl(s)g(t-s)dsmentioning
confidence: 99%
“…The function a(p', x') is the « symplectic Fourier transform » of a(x, p) [2]. It results from a special identification between the dual of R 2 " and R 2 " itself.…”
Section: The Weyl Correspondencementioning
confidence: 99%
“…We shall now exhibit the irreducible sector lo{h) (which is denoted by 3^ in [4] and [2]). Consider the gaussian To end this section, we mention how the unitary equivalences between, for instance, the representations (a), (?)…”
Section: If F and G Belong To L^rmentioning
confidence: 99%
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