2017
DOI: 10.1088/1751-8121/50/32/323001
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GeneralizedSU(2) covariant Wigner functions and some of their applications

Abstract: We survey some applications of SU(2) covariant maps to the phase space quantum mechanics of systems with fixed or variable spin. A generalization to SU(3) symmetry is also briefly discussed in framework of the axiomatic Stratonovich-Weyl formulation.

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Cited by 52 publications
(59 citation statements)
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“…We also think that similar features hold far beyond the two elementary symmetries which have been examined here. There exist many versions of the Wigner function or equivalent quasi-distribution for other groups, see for instance [ 39 , 40 ] for SU and references therein. In the case of non-compact groups, particularly those which are semi-direct products of groups, the existence of square-integrability of the UIR requested by the resolution of the identity lying at the heart of the construction is in general not guaranteed.…”
Section: Discussionmentioning
confidence: 99%
“…We also think that similar features hold far beyond the two elementary symmetries which have been examined here. There exist many versions of the Wigner function or equivalent quasi-distribution for other groups, see for instance [ 39 , 40 ] for SU and references therein. In the case of non-compact groups, particularly those which are semi-direct products of groups, the existence of square-integrability of the UIR requested by the resolution of the identity lying at the heart of the construction is in general not guaranteed.…”
Section: Discussionmentioning
confidence: 99%
“…The exact evolution equation for W (s) ρ (Ω) has been derived in [59] (see also [60] and [61], where the corresponding starproduct for the map is discussed). In most physical applications only Hamiltonians quadratic in the spin generators play an important role.…”
Section: Hamiltonian Dynamics and Currents On The Spherementioning
confidence: 99%
“…The representation of Kraus operators E a i for this channel [25] is given by, According to Eqs. (5), (11)and (7), the final output state that passes through C bf is given by,…”
Section: The Bit Flip Channel C Bfmentioning
confidence: 99%
“…[5] investigated analytically the Wigner function distribution of a two-qubit field system in the presence of pure phase noisy. The s-parameterized Q − P D is described in the angular momentum basis via atomic coherent state [6,7]. However, the value of s-parameters determines the type of the Q − P D, where s = −1, 0, 1, represent the Husimi-Berezin Q-function, [8,9], Wigner quasi-distribution function [10,11], and the P -function [12], respectively.…”
Section: Introductionmentioning
confidence: 99%
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