Abstract

We derive a continuity equation for the evolution of the SU(2) Wigner function under nonlinear Kerr evolution. We give explicit expressions for the resulting quantum Wigner current, and discuss the appearance of the classical limit. We show that the global structure of the quantum current significantly differs from the classical one, which is clearly reflected in the form of the corresponding stagnation lines.

Highlights

  • An ensemble of particles is described by a distribution function f (x, p|t) that depends on the phase-space variables x and p and evolves in time

  • Wρ (Ω|t) Wρ (Ω(−t)|0), where Ω(t) are classical trajectories generated by WH (Ω). It has been pointed out [16,17,18], that one can construct a Wigner current ‡ in such a way that the evolution can be mapped as a continuity equation very much analogous to (1.1)

  • The form of the current, and especially the behavior in the vicinity of its stagnation points, can be used for the characterization of the quantumness of the evolution. We extend these ideas to spinlike systems, where the classical phase space is the unit sphere

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Summary

Introduction

An ensemble of particles is described by a distribution function f (x, p|t) that depends on the phase-space variables x and p and evolves in time. Wρ (Ω|t) Wρ (Ω(−t)|0), where Ω(t) are classical trajectories generated by WH (Ω) It has been pointed out [16,17,18], that one can construct a Wigner current ‡ in such a way that the evolution can be mapped as a continuity equation very much analogous to (1.1). We will show, using the simplest example of nonlinear Kerr dynamics, that the global structure of the quantum Wigner current significantly differs from the classical one Such a difference is clearly observable even during the short-time evolution of semiclassical states (specified by localized distributions in phase space), when the Wigner distribution can still be well described in terms of the semiclassical approximation. An extra benefit of bringing the Wigner current into play is that it can give a compelling visual representation of how nonclassical features arise during the evolution

Wigner function on the sphere
Dynamics and Wigner current on the sphere
Linear Hamiltonians
Kerr dynamics
Semiclassical limit
Concluding remarks
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