1981
DOI: 10.1002/andp.19814930110
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Statistics of a Stokes‐Antistokes Interacting Boson System with Damping

Abstract: The statistics of a system of four boson modes in Stokes-Antistokes interaction is considered with respect to the influence of damping in one mode. The time evolution of the system is calculated. The mean particle numbers and the factorial moments of photon number distribution are calculated. Sunierical results show strong dependence on bath temperature but only weak influence of the bath coupling strength. In the combined Stokes-Antistokes system Antibunching appears if the bath temperature is low.

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Cited by 7 publications
(5 citation statements)
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“…The present paper is a continuation of the work presented in [5], where a general description of the quantum statistics in Brillouin scattering were proposed based on the coherent-state technique . Recently, similar models for Raman scattering have been discussed in [6][7][8][9][10] . In [6], Peiina described the phonons as an infinite markoffian reservoir system whose variables have been eliminated in the process of calculation .…”
Section: Introductionmentioning
confidence: 93%
“…The present paper is a continuation of the work presented in [5], where a general description of the quantum statistics in Brillouin scattering were proposed based on the coherent-state technique . Recently, similar models for Raman scattering have been discussed in [6][7][8][9][10] . In [6], Peiina described the phonons as an infinite markoffian reservoir system whose variables have been eliminated in the process of calculation .…”
Section: Introductionmentioning
confidence: 93%
“…As a digression, let us mention that the same phenomenological Hamiltonians (2) have been used in the description of Brillouin scattering (see, for example, Refs. [105,180] and [23] and references therein). The main difference between Brillouin and Raman scattering lies in different kinds of the scatterers responsible for these effects: acoustic phonons in the Brillouin effect, and optical phonons in the Raman effect.…”
Section: Model and Master Equationmentioning
confidence: 99%
“…Refs. [23,105,145]), where optical phonons are included in the system, whereas other crystal excitation modes, such as acoustical phonons, electric excitations, and other species of molecular vibrations, serve as a thermal reservoir. The radiation fields are weakly coupled to the thermal reservoir.…”
Section: Model and Master Equationmentioning
confidence: 99%
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