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The Berezin–Simon (BS) quantization is a rigorous version of the ``operator formalism’’ of quantization procedure. The goal of the paper is to present a rigorous real-time (not imaginary-time) path-integral formalism corresponding to the BS operator formalism of quantization; Here we consider the classical systems whose phase space is a (possibly non-compact) Kähler manifold which satisfies some conditions, with a Hamiltonian . For technical reasons, we consider only the cases where is smooth and bounded. We use Güneysu’s extended version of the Feynman–Kac theorem to formulate the path-integral formula.

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