Contact Geometry and Quantum Mechanics
arXiv:1709.04557 · doi:10.1016/j.physletb.2018.04.008
Abstract
We present a generally covariant approach to quantum mechanics in which generalized positions, momenta and time variables are treated as coordinates on a fundamental "phase-spacetime." We show that this covariant starting point makes quantization into a purely geometric flatness condition. This makes quantum mechanics purely geometric, and possibly even topological. Our approach is especially useful for time-dependent problems and systems subject to ambiguities in choices of clock or observer. As a byproduct, we give a derivation and generalization of the Wigner functions of standard quantum mechanics.
arXiv comment7 pages, 1 figure, LaTeX, references added, journal version
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