Induced Gauge Fields in the Path Integral
arXiv:hep-th/9508165 · doi:10.1142/S021773239500274X
Abstract
The path integral on a homogeneous space is constructed, based on the guiding principle `first lift to and then project to '. It is then shown that this principle admits inequivalent quantizations inducing a gauge field (the canonical connection) on the homogeneous space, and thereby reproduces the result obtained earlier by algebraic approaches.
12 pages, no figures, LaTeX
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