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.Comment: Updated version. Phys. Rev. A (in press