2011
DOI: 10.1007/s00220-011-1230-0
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Distortion of the Poisson Bracket by the Noncommutative Planck Constants

Abstract: In this paper we introduce a kind of "noncommutative neighbourhood" of a semiclassical parameter corresponding to the Planck constant. This construction is defined as a certain filtered and graded algebra with an infinite number of generators indexed by planar binary leaf-labelled trees. The associated graded algebra (the classical shadow) is interpreted as a "distortion" of the algebra of classical observables of a physical system. It is proven that there exists a q-analogue of the Weyl quantization, where q … Show more

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Cited by 5 publications
(16 citation statements)
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“…Let us now go back to the analogy between the semiclassical quantum mechanics and the quasithermodynamic statistical physics discussed in the introduction. This paper is a natural continuation of [1]. It is important to stress, that in order to construct a reasonable q-analogue of a classical theory (mechanics or thermodynamics), it is not enough just to apply the q-analysis (replacing derivatives with q-derivatives, factorials with q-factorials, etc.).…”
Section: Discussionmentioning
confidence: 99%
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“…Let us now go back to the analogy between the semiclassical quantum mechanics and the quasithermodynamic statistical physics discussed in the introduction. This paper is a natural continuation of [1]. It is important to stress, that in order to construct a reasonable q-analogue of a classical theory (mechanics or thermodynamics), it is not enough just to apply the q-analysis (replacing derivatives with q-derivatives, factorials with q-factorials, etc.).…”
Section: Discussionmentioning
confidence: 99%
“…It is necessary to introduce the Planck-Boltzmann constants → 0 or k B → 0 into the theory first. The paper [1] is focused on → 0, and starts with an investigation of a q-analogue of the Weyl quantization map in quantum mechanics. In the non-q-deformed case this is just a symmetrization map linking the classical coordinates x and momenta p, with the quantized coordinates and momenta x and p. Trying to construct a reasonable q-analogue of such symmetrization map in case q is a 2s × 2s matrix of formal variables (2) defining the braidings (3) on the phase space (where s is the number of degrees of freedom), one realizes that the Planck constant should acquire indices, → i,j , i, j ∈ [2s], and should have same commutation properties as the q-commutator…”
Section: Discussionmentioning
confidence: 99%
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