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Deformation Quantization: Quantum Mechanics Lives and Works in Phase-Space
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Wigner's quasi-probability distribution function in phase-space is a special (Weyl) representation of the density matrix. It has been useful in describing quantum transport in quantum optics; nuclear physics; decoherence (eg, quantum computing); quantum chaos; "Welcher Weg" discussions; semiclassical limits. It is also of importance in signal processing. Nevertheless, a remarkable aspect of its internal logic, pioneered by Moyal, has only emerged in the last quarter-century: It furnishes a third, alternative, formulation of Quantum Mechanics, independent of the conventional Hilbert Space, or Path Integral formulations. In this logically complete and self-standing formulation, one need not choose sides--coordinate or momentum space. It works in full phase-space, accommodating the uncertainty principle. This is an introductory overview of the formulation with simple illustrations.
Forward citations
Cited by 4 Pith papers
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The Feynman-Kac formula in deformation quantization
The ground state energy of a quantum system is extracted from the large imaginary-time limit of the phase space integral of the star exponential of the Hamiltonian, a reformulation of the trace formula.
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Wigner function under changes of reference frames
Under unitary reference-frame changes that map position to X(x) and momentum to P(p), the Wigner function transforms by an explicit integral formula, reducing to W(X,P) in the affine examples shown.
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