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WORLD SCIENTIFIC (EUROPE) eBooks

The Moyal Identity

Published Mar 27, 2017• 0 citations
Publisher
DOI
10.1142/9781786343109_0006

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This simple example is used to show how the formalism of Moyal works when it is applied to systems of identical particles. The symmetric and antisymmetric Moyal propagators are evaluated for this case; from them, the correct energy levels of energy are obtained, as well as the Wigner functions for the symmetric and antisymmetric states of the two identical particle system. Finally, the solution of the Bloch equation is straightforwardly obtained from the expressions of the Moyal propagators.

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Notes on qubit phase space and discrete symplectic structures

Etera R. Livine

We start from Wootter's construction of discrete phase spaces and Wigner functions for qubits and more generally for finite-dimensional Hilbert spaces. We look at this framework from a non-commutative space perspective and we focus on the Moyal product and the differential calculus on these discrete phase spaces. In particular, the qubit phase space provides the simplest example of a four-point non-commutative phase space. We give an explicit expression of the Moyal bracket as a differential operator. We then compare the quantum dynamics encoded by the Moyal bracket to the classical dynamics: we show that the classical Poisson bracket does not satisfy the Jacobi identity thus leaving the Moyal bracket as the only consistent symplectic structure. We finally generalize our analysis to Hilbert spaces of prime dimensions d and their associated d × d phase spaces.

arXiv:0906.4516•Journal of Physics A Mathematical and Theoretical•Jan 29, 2010•11 citations

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On the Moyal Formulation of Quantum Identical Particles

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Wigner functions of permutation operators are obtained and are used as a basis for a phase space formulation of quantum identical particles. Non-spin systems as well as 1/2 spin systems are considered. The general results are applied to a couple of examples.

Fortschritte der Physik/Progress of Physics•Jan 1, 1994•4 citations
We start from Wootter's construction of discrete phase spaces and Wigner functions for qubits and more generally for finite-dimensional Hilbert spaces. We look at this framework from a non-commutative space perspective and we focus on the Moyal product and the differential calculus on these discrete phase spaces. In particular, the qubit phase space provides the simplest example of a four-point non-commutative phase space. We give an explicit expression of the Moyal bracket as a differential operator. We then compare the quantum dynamics encoded by the Moyal bracket to the classical dynamics: we show that the classical Poisson bracket does not satisfy the Jacobi identity thus leaving the Moyal bracket as the only consistent symplectic structure. We finally generalize our analysis to Hilbert spaces of prime dimensions d and their associated d × d phase spaces.