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
Summary
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
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.