2021
DOI: 10.1007/s13538-020-00848-6
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Nonlocal Theory of Excitation of Electron Bernstein Waves by a Relativistic Electron Beam in Plasma with Loss-Cone Distribution of Electron

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Cited by 18 publications
(4 citation statements)
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“…The electron Bernstein wave is a particular type of electron cyclotron harmonic with electrostatic characteristics. This electrostatic wave can be excited by the interaction of an electron beam with plasma and the interaction of a laser beam with plasma as well as clustered plasma with a static magnetic field [30][31][32]. The association of an electron Bernstein wave with an extraordinary laser beam causes enhanced second and third harmonic generations in plasma [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…The electron Bernstein wave is a particular type of electron cyclotron harmonic with electrostatic characteristics. This electrostatic wave can be excited by the interaction of an electron beam with plasma and the interaction of a laser beam with plasma as well as clustered plasma with a static magnetic field [30][31][32]. The association of an electron Bernstein wave with an extraordinary laser beam causes enhanced second and third harmonic generations in plasma [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…In laser‐plasma experiments, laser frequency nonlinearly couples with the EBW frequency (pre‐existed) which gives rise to laser‐beam absorption in the plasma. In Reference [11] authors studied EBW excitation by a relativistic electron beam with loss‐cone distribution of electrons in plasma and reported that EBWs are absorbed efficiently by the electrons in the region where its frequency matches with electron cyclotron frequency. Such physical mechanisms can contribute to plasma heating.…”
Section: Introductionmentioning
confidence: 99%
“…Many groups have theoretically proposed the non-local theory of electron Bernstein wave excitation by the method of non-relativistic electron beams [30], gyrating relativistic electron beams [31], and relativistic electron beams with loss cone-velocity distribution [32] in plasma. The counterpropagation of two laser beams in the plasmas resonantly excites the fast and slow plasma wave.…”
Section: Introductionmentioning
confidence: 99%