2009
DOI: 10.1063/1.3176616
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Temperature effects on the nonstationary Karpman–Washimi ponderomotive magnetization in quantum plasmas

Abstract: The temperature effects on the nonstationary Karpman–Washimi ponderomotive magnetization are investigated in quantum Fermi plasmas. The cyclotron frequency due to the ponderomotive force of the electromagnetic wave has been obtained as a function of the Fermi Debye length and quantum wavelength. It is found that the Karpman–Washimi ponderomotive magnetization decreases with increasing Fermi temperature. The maximum position of the Fermi Debye length is found to be increased with an increase in the frequency in… Show more

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Cited by 26 publications
(6 citation statements)
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“…Considering the quantum mechanical effect, the Fermi gas pressure and the Bohm potential, the dielectric constant for unmagnetized and collisionless thermal quantum plasma takes this form [52,57]:…”
Section: Theorymentioning
confidence: 99%
See 1 more Smart Citation
“…Considering the quantum mechanical effect, the Fermi gas pressure and the Bohm potential, the dielectric constant for unmagnetized and collisionless thermal quantum plasma takes this form [52,57]:…”
Section: Theorymentioning
confidence: 99%
“…The self-focusing of an intense laser beam in the classical plasma and in the cold quantum plasma has been studied by considering different plasma density profiles [49][50][51][52]. In the thermal homogenous quantum plasma, the laser selffocusing effect has been investigated by Patil et al [48].…”
Section: Introductionmentioning
confidence: 99%
“…We have considered the plasma dielectric function in the relativistic manner for unmagnetized and collisionless CQP in the following form [65], [66]:…”
Section: Self-focusing Of Chg Laser Beam: Off-axis Contributionmentioning
confidence: 99%
“…The nonlinear and saturating character of the dielectric permittivity in the collisionless and collisional quantum plasma has been caused to some interesting features in the propagation of the laser beam. 24,49,50,[65][66][67][68] Therefore, in this paper, we have considered the plasma dielectric function for unmagnetized and collisionless WQP in the following form: 49 e r; z ð Þ ¼ 1 À…”
Section: Beam-width Parameter Evolutionmentioning
confidence: 99%
“…Temperature effects are also included in dense degenerate plasma via a warm quantum model. 49,50 Arista and Brandt 51 have calculated the dielectric function e k; x ð Þ of an electron plasma in thermal equilibrium for all degrees of plasma degeneracy. They have incorporated thermal and quantum effects on e k; x ð Þ, and included the results from classical and semi-classical approximations as well as those of quantum calculations for the degenerate plasma.…”
mentioning
confidence: 99%