1989
DOI: 10.1016/0003-4916(89)90262-5
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The moyal representation for spin

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Cited by 277 publications
(338 citation statements)
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“…[46,47]). One practical and formally justified [48,49] axiomatic basis for algorithm (II) postulates the equations of motion for averages of certain physical quantities [38,50].…”
Section: The Fundamentals Of Generalized Wigner Representationsmentioning
confidence: 99%
“…[46,47]). One practical and formally justified [48,49] axiomatic basis for algorithm (II) postulates the equations of motion for averages of certain physical quantities [38,50].…”
Section: The Fundamentals Of Generalized Wigner Representationsmentioning
confidence: 99%
“…Faure and Zhilinskii use the pre-factor 1 j , instead of 2 dj , in front of the coupling term J · S. But, the factor 1 dj turns out to be the expansion parameter of the -product to be introduced in this context 29,30,49 , and is therefore better suited for our purposes 50 . Anyway, in the (adiabatic) limit j → ∞, the difference of the two factors becomes negligible.…”
Section: A Model With Non-commutative Slow Variables: Spin-orbit mentioning
confidence: 99%
“…In principle, we can also define a Berezin--product for a spin coherent state quantisation of the scale of Poisson algebras C ∞ (S 2 ) = dj ∈N C ∞ dj (S 2 ), because a closed de-quantisation formula, similar to (4.3), exists 30,42 . A d j -expansion of this -product is arrived at via an easy, but extremely tedious, calculation along the lines of 49 .…”
Section: Remark Iv1mentioning
confidence: 99%
“…takes values in the hermitian 2 × 2 matrices, see [VGB89]. The quantisers ∆ 1/2 (n) provide a quantum-classical correspondence on the sphere that is covariant with respect to SU(2)-rotations in the following sense,…”
Section: Classical Limit Of Quantum Dynamicsmentioning
confidence: 99%