Path distributions for describing eigenstates of orbital angular momentum
Abstract
The manner in which probability amplitudes of paths sum up to form wave functions of orbital angular momentum eigenstates is described. Using a generalization of stationary-phase analysis, distributions are derived that provide a measure of how paths contribute towards any given eigenstate. In the limit of long travel-time, these distributions turn out to be real-valued, non-negative functions of a momentum variable that describes classical travel between the endpoints of a path (with the paths explicitly including nonclassical ones, described in terms of elastica). The distributions are functions of both this characteristic momentum as well as a polar angle that provides a tilt, relative to the z-axis of the chosen coordinate system, of the geodesic that connects the endpoints. The resulting description provides a replacement for the well-known "vector model" for describing orbital angular momentum, and importantly, it includes treatment of the case when the quantum number is zero (i.e., s-states).
Keywords
Cite
@article{arxiv.2308.02884,
title = {Path distributions for describing eigenstates of orbital angular momentum},
author = {Randall M. Feenstra},
journal= {arXiv preprint arXiv:2308.02884},
year = {2025}
}
Comments
In both v6 and v7, revisions were made in Section II(F) and Appendix III such that the angular length of the elastica was referred to rather than the arc length (product of angular length times radius of curvature). Changes in Eqs. (48) and (49) resulted. The final results for path distributions were unaffected. Computer codes were added in v7