Quantization of the linearly damped harmonic oscillator

H. Dekker
Phys. Rev. A 16, 2126 – Published 1 November 1977; Erratum Phys. Rev. A 17, 1240 (1978)
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Abstract

A previously developed novel theory for the formal canonical quantization of classically dissipating systems will be the starting point for a detailed discussion of the quantum statistical aspects of the simple linearly damped harmonic oscillator. The formalism essentially involves complex classical canonical coordinates and momenta, and thus quite naturally leads to the possibility of creation and annihilation operators. Furthermore, the occurrence of quantal noise operators appears to be of principal importance for the conservation of the fundamental commutator in the course of time, as will be expressed in a simple fluctuation-dissipation relation. Making a canonical transformation back to the real, Cartesian Hermitian position and momentum an "effective" Hermitian Hamiltonian will be derived, with which a transformation is made from the Heisenberg frame to the Schrödinger frame where the density operator equation will be computed. This will make it obvious that no proper Schrödinger equation exists for the dissipative subsystem on its own, thus reflecting an incomplete knowledge. The master equation will then be translated into its Wigner representation. The intimate connection between the diffusion coefficients in the resulting Fokker-Planck equation and the uncertainty relation will be demonstrated in a clear fashion.

  • Received 8 June 1977

DOI:https://doi.org/10.1103/PhysRevA.16.2126

©1977 American Physical Society

Erratum

Authors & Affiliations

H. Dekker*

  • Physics Laboratory TNO, Den Haag, The Netherlands

  • *P. O. Box 2864.

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Issue

Vol. 16, Iss. 5 — November 1977

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