Abstract

We address the time evolution of two- and three-dimensional nonrelativistic Gaussian wave packets in the presence of a weak external potential of arbitrary functional form. The focus of our study is the phenomenon of rotation of a Gaussian wave packet around its center of mass, as quantified by mean angular momentum computed relative to the wave packet center. Using a semiclassical approximation of the eikonal type, we derive an explicit formula for a time-dependent change of mean angular momentum of a wave packet induced by its interaction with a weak external potential. As an example, we apply our analytical approach to the scenario of a two-dimensional quantum particle crossing a tilted ridge potential barrier. In particular, we demonstrate that the initial orientation of the particle wave packet determines the sense of its rotation, and report a good agreement between analytical and numerical results.

Highlights

  • Among many motivations to study the time evolution of quantum matter-wave packets two are noteworthy

  • In this paper we have analyzed the phenomenon of internal rotation of two- and three-dimensional quantum Gaussian wave packets in the presence of weak external potentials

  • Using semiclassical analysis, we have obtained an explicit expression, given by Eqs. (44) and (47), for the internal mean angular momentum of a Gaussian wave packet propagating through an arbitrary weak external potential

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Summary

INTRODUCTION

Among many motivations to study the time evolution of quantum matter-wave packets two are noteworthy. Of particular interest to the present work is a recent paper by Dodonov [14], in which the author addresses the time evolution of nonrelativistic two-dimensional Gaussian wave packets possessing a finite value of mean angular momentum (MAM) [22,23]. Using a semiclassical (short-wavelength) approximation to the full quantum-mechanical propagator, we obtain an explicit formula that gives the value of the internal MAM as a function of the propagation time, parameters of the initial wave packet, and the external potential. But technically strenuous calculations are deferred to the Appendixes

PROPAGATION OF GAUSSIAN WAVE PACKETS IN WEAK EXTERNAL POTENTIALS
Free particle motion
Eikonal-type approximation
MEAN ANGULAR MOMENTUM
Gaussian wave packet
Eikonal wave packet
EXAMPLE SYSTEM
Analytics
Numerics
SUMMARY AND CONCLUSIONS

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