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Physica Scripta

On the asymptotic solutions of Belavkin's stochastic wave equation

Dariusz Chruściński, P. Staszewski

Published Mar 1, 1992• 38 citations
Publisher

Abstract

A posterior dynamics of an observed quantum particle in a quadratic potential is studied. It is proved that Belavkin's stochastic wave equation for the quantum particle with continuously observed 1) position, 2) momentum, 3) position and momentum is uniquely relaxing to the corresponding Gaussian wave packet for any initial square-integrable wave function. A comparison of the asymptotic position-momentum uncertainties of these measurements is given.

DOI
10.1088/0031-8949/45/3/001

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A posterior dynamics of an observed quantum particle in a quadratic potential is studied. It is proved that Belavkin's stochastic wave equation for the quantum particle with continuously observed 1) position, 2) momentum, 3) position and momentum is uniquely relaxing to the corresponding Gaussian wave packet for any initial square-integrable wave function. A comparison of the asymptotic position-momentum uncertainties of these measurements is given.
We analyze the time-behaviour of the Gaussian wave packet of a quantum particle moving in the field of a linear force, undergoing a continuous nondemolition observation of its position. In particular, the time-dependence of position and momentum dispersions, as well as position-momentum uncertainty is investigated. The discussion includes the case of a free particle and initially coherent state of a harmonic oscillator. It is found that in the beginning of observation the momentum dispersion and position-momentum uncertainty always increase in contrast to the position dispersion. It is also proved that all considered functions asymptotically take the form of harmonic oscillations, decaying to finite values. For initially coherent states, the asymptotic bounds for all considered functions are given.
A stochastic Schrödinger equation is presented to describe simultaneous continuous measurement of the position and momentum of a non-relativistic particle. The equation is solved to yield a state localised in position and momentum contingent on the uncertainty principle. The state is understood as that to which the particle tends after a period of continuous measurement. The solution takes the form of a wave packet of fixed Gaussian shape whose centre undergoes random motion in phase space. It is shown to be locally stable.
A stochastic model of a continuous nondemolition observation of a quantum system is presented. The nonlinear stochastic wave equation describing the posterior dynamics of the observed quantum system is solved for a free particle of mass m>0. It is shown that the dispersion of the Gaussian wave packet does not increase to infinity as for a free unobserved particle, but tends to the finite limit ${\mathrm{\ensuremath{\tau}}}_{\mathrm{\ensuremath{\infty}}}^{2}$=(\ensuremath{\Elzxh}/2\ensuremath{\lambda}m)1/2{)}^{1/2})1/2, where \ensuremath{\lambda} is the accuracy coefficient of an indirect nondemolition measurement of the particle's position.
Recently, the stochastic nonlinear wave equation describing the dynamics of an observed quantum system has been solved for a free particle [Phys. Rev. A 45, 1347 (1992)]. In this paper, transient effects that occur during a continuous observation of the particle position are discussed. It is shown that the dispersion of the Gaussian wave packet of the particle always decreases in the beginning of the observation, then takes the form of oscillations which, after a short time, decay rapidly to the asymptotic value.
The paper deals with the quantum Langevin equation describing a quantum particle with continuously observed position. Special Banach spaces of entire analytic functions are introduced and studied (including a theorem of Paley–Wiener type for them), which comprise all solutions of this equation and in which the uniform convergence (as time tends to infinity) of the solutions to the Gaussian function with a fixed dispersion (selflocalisation or continuous collapse) is proved. The asymptotic behavior at infinity of the mean position and momentum of the limit Gaussian wave packet (which satisfy classical Langevin equations) is also investigated.