Abstract

We investigate a class of operators resulting from a quantization scheme attributed to Berezin. These so-called Berezin–Toeplitz operators are defined on a Hilbert space of square-integrable holomorphic sections in a line bundle over the classical phase space. As a first goal we develop self-adjointness criteria for Berezin–Toeplitz operators defined via quadratic forms. Then, following a concept of Daubechies and Klauder, the semigroups generated by these operators may under certain conditions be represented in the form of Wiener-regularized path integrals. More explicitly, the integration is taken over Brownian motion paths in phase space in the ultra-diffusive limit. All results are the consequence of a relation between Berezin–Toeplitz operators and Schrödinger operators defined via certain quadratic forms. The probabilistic representation is derived in conjunction with a version of the Feynman–Kac formula.

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