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Random Quantization of Hamiltonian Systems

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Abstract

A quantization of a Hamiltonian system is an ambiguous procedure. Accordingly, we introduce the notion of random quantization, related random variables with values in the set of self-adjoint operators, and random processes with values in the group of unitary operators. The procedures for the averaging of random unitary groups and averaging of random self-adjoint operators are defined. The generalized weak convergence of a sequence of measures and the corresponding generalized convergence in distribution of a sequence of random variables are introduced. The generalized convergence in distribution for some sequences of compositions of random mappings is obtained. In the case of a sequence of compositions of shifts by independent random vectors of Euclidean space, the obtained convergence coincides with the statement of the central limit theorem for a sum of independent random vectors. The results are applied to the dynamics of quantum systems arising in random quantization of a Hamiltonian system.

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Funding

John Gough acknowledges funding by the French National Research Agency under the grant Q-COAST ANR-19-CE48-0003.

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Correspondence to V. Zh. Sakbaev.

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Translated by I. Ruzanova

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Gough, J., Orlov, Y.N., Sakbaev, V.Z. et al. Random Quantization of Hamiltonian Systems. Dokl. Math. 103, 122–126 (2021). https://doi.org/10.1134/S106456242103008X

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  • DOI: https://doi.org/10.1134/S106456242103008X

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