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Proceedings of the Samahang Pisika ng Pilipinas

Commutation relations for simplest symmetric ordering of position and inverse momentum operators

Herbert B. Domingo, Eric A. Galapon

Published Oct 17, 2014• 0 citations
OpenAlex

Abstract

Quantization under simplest symmetric ordering of classical monomials with negative integral exponents of momentum has been written in integral form. This integral representation not only proved useful in transforming Weyl quantization to symmetric ordering quantization, and vice versa. They also facilitate derivation of commutation relations among different operators involving inverse powers of momentum operator, relations which can be used in solving quantization problems for classical functions with singularity along the momentum axis.

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Quantization under simplest symmetric ordering of classical monomials with negative integral exponents of momentum has been written in integral form. This integral representation not only proved useful in transforming Weyl quantization to symmetric ordering quantization, and vice versa. They also facilitate derivation of commutation relations among different operators involving inverse powers of momentum operator, relations which can be used in solving quantization problems for classical functions with singularity along the momentum axis.
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In this paper, it can be found that there is a type of integra-transformation which corresponds to a quantum mechanical fundamental commutative relation, with its integral kernel being 1/exp[2i(q-Q)(p-P)], here denotes Weyl ordering, and Q and P are the coordinate and the momentum operator, respectively. Such a transformation is responsible for the mutual-converting among three ordering rules(P-Q ordering, Q-P ordering and Weyl ordering). We also deduce the relationship between this kernel and the Wigner operator, and in this way a new approach for deriving Wigner function in quantum states is obtained.
The commutator of position and momentum operators is first considered in the coordinate and momentum representations, and then in an abstract Hilbert space. The reader is then introduced to canonical operators with the associated canonical quantization of commutation rules, which consists of maps defined on a symplectic space and taking values in the set of unitary operators on a Hilbert space. If the symplectic space is finite-dimensional, all of its irreducible representations are unitarily equivalent. The Weyl exponentiated form of the commutation relations is described and investigated. One then arrives at the definition of Weyl systems, and it is shown how to recover from them the formulation in terms of self-adjoint operators which satisfy a generalized form of commutation relations. Further topics are the Heisenberg representation for temporal evolution and the generalized uncertainty relations. Unitary operators associated with symplectic linear transformations are then considered, and, within this framework, translations, rotations and the harmonic oscillator are considered. The Weyl programme is then reassessed. Lastly, the basic postulates of modern quantum theory are eventually studied: the probabilistic nature of the predictions of results of measurements; the correspondence between observables and self-adjoint operators on Hilbert spaces; the expected result of measuring an observable quantity; and the evolution of the state vector in systems which are not affected by any external influence. The chapter ends with an outline of rigged Hilbert space formalism and its applications. The commutator in wave mechanics In the first part of this book we studied wave mechanics within the framework of the Schrödinger equation.