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Polar Coordinates and Noncommutative Phase Space

The so-called Weyl transform is a linear map from a commutative algebra of functions to a noncommutative algebra of linear operators, characterized by an action on Cartesian coordinate functions of the form $(x, y) \mapsto (X, Y)$ such that $XY -YX = iεI$, i.e. the defining relation for the Heisenberg Lie algebra. Study of this transform has been expansive. We summarize many important results from the literature. The primary goal of this work is to prove the final result: the realization of the polar transformation $(ρ, e^{iθ}) \mapsto (R, e^{iΘ})$ in terms of explicit orthogonal function expansions, while starting from elementary principles and utilizing minimal machinery. Our results are not strictly original but their presentation here is intended to simplify introduction to these subjects in a novel manner.