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Title: Anomalous fluctuations in an electron system with a nonparabolic energy dispersion relation

Abstract

A quantum approach is proposed for the study of electromagnetic fluctuations in an electron plasma in an external radiation field. The electrons are assumed to obey a nonparabolic energy dispersion relation. It is shown that the fluctuation amplitudes increase anomalously near the limit of parametric instability.

Authors:
;
Publication Date:
OSTI Identifier:
5972864
Alternate Identifier(s):
OSTI ID: 5972864
Resource Type:
Journal Article
Journal Name:
Sov. Phys. - Solid State (Engl. Transl.); (United States)
Additional Journal Information:
Journal Volume: 21:2
Country of Publication:
United States
Language:
English
Subject:
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; SOLID-STATE PLASMA; DISPERSION RELATIONS; FLUCTUATIONS; INSTABILITY; PLASMA; VARIATIONS 656001* -- Condensed Matter Physics-- Solid-State Plasma

Citation Formats

Chong, N.V., and Dat, N.N. Anomalous fluctuations in an electron system with a nonparabolic energy dispersion relation. United States: N. p., 1979. Web.
Chong, N.V., & Dat, N.N. Anomalous fluctuations in an electron system with a nonparabolic energy dispersion relation. United States.
Chong, N.V., and Dat, N.N. Thu . "Anomalous fluctuations in an electron system with a nonparabolic energy dispersion relation". United States.
@article{osti_5972864,
title = {Anomalous fluctuations in an electron system with a nonparabolic energy dispersion relation},
author = {Chong, N.V. and Dat, N.N.},
abstractNote = {A quantum approach is proposed for the study of electromagnetic fluctuations in an electron plasma in an external radiation field. The electrons are assumed to obey a nonparabolic energy dispersion relation. It is shown that the fluctuation amplitudes increase anomalously near the limit of parametric instability.},
doi = {},
journal = {Sov. Phys. - Solid State (Engl. Transl.); (United States)},
number = ,
volume = 21:2,
place = {United States},
year = {1979},
month = {2}
}