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We canonically quantize a Poisson manifold to a Lie 2-groupoid, complete with a quantization map, and show that it relates geometric and deformation quantization: the perturbative expansion in of the (formal) convolution of two quantized functions yields Kontsevich's star product. Meanwhile, we can push forward this quantization map (by integrating over homotopies of paths) to obtain a quantization map in traditional geometric quantization. This gives a polarization-free, path integral definition of the quantization map, which does not have a prior definition for Poisson manifolds, and which only has a partial prescription for symplectic manifolds. We construct conventional quantum mechanics from this perspective.
Joshua Lackman (Thu,) studied this question.
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