2002
DOI: 10.1134/1.1463114
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Dissipation of strong Langmuir turbulence in nonisothermal non-Maxwellian plasma

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Cited by 21 publications
(5 citation statements)
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“…The supersonic MI, which is popularly known as the oscillating two stream instability (OTSI) [ Papadopoulos et al , 1974; Smith et al , 1979; Goldstein et al , 1979] and, soliton formation and Langmuir collapse [ Zakharov , 1972; Nicholson et al , 1978; Goldman , 1983] are suggested as the most effective beam stabilization mechanisms. These strong Langmuir turbulence processes are the focus of several theoretical studies [ Zakharov , 1972; Goldman , 1984; Robinson , 1997], computer simulations [ Bardwell and Goldman , 1976; Nicholson et al , 1978; Degtyarev et al , 1980; Doolen et al , 1985; Russell et al , 1988] and experimental investigations [ Whelan and Stenzel , 1981; Michel et al , 1982; Wong and Cheung , 1984; Cheung and Wong , 1985a, 1985b; McFarland and Wong , 1997, 2001; Vyacheslavov et al , 2002] because of the fundamental nature of the problem [ Zakharov , 1972; Krasnoselskikh and Sotnikov , 1977], and practical importance in fields, such as the laser heating of pellets [ Montgomery et al , 1999], ionospheric modification experiments [ DuBois et al , 1993], and several astrophysical applications [ Galeev and Krasnoselskikh , 1976, 1978; Gurnett et al , 1981; Pelletier et al , 1988; Balikhin et al , 1989; Kellogg et al , 1999].…”
Section: Introductionmentioning
confidence: 99%
“…The supersonic MI, which is popularly known as the oscillating two stream instability (OTSI) [ Papadopoulos et al , 1974; Smith et al , 1979; Goldstein et al , 1979] and, soliton formation and Langmuir collapse [ Zakharov , 1972; Nicholson et al , 1978; Goldman , 1983] are suggested as the most effective beam stabilization mechanisms. These strong Langmuir turbulence processes are the focus of several theoretical studies [ Zakharov , 1972; Goldman , 1984; Robinson , 1997], computer simulations [ Bardwell and Goldman , 1976; Nicholson et al , 1978; Degtyarev et al , 1980; Doolen et al , 1985; Russell et al , 1988] and experimental investigations [ Whelan and Stenzel , 1981; Michel et al , 1982; Wong and Cheung , 1984; Cheung and Wong , 1985a, 1985b; McFarland and Wong , 1997, 2001; Vyacheslavov et al , 2002] because of the fundamental nature of the problem [ Zakharov , 1972; Krasnoselskikh and Sotnikov , 1977], and practical importance in fields, such as the laser heating of pellets [ Montgomery et al , 1999], ionospheric modification experiments [ DuBois et al , 1993], and several astrophysical applications [ Galeev and Krasnoselskikh , 1976, 1978; Gurnett et al , 1981; Pelletier et al , 1988; Balikhin et al , 1989; Kellogg et al , 1999].…”
Section: Introductionmentioning
confidence: 99%
“…The strong turbulence theory ignores the wave-particle effect, and is a macroscopic theory. Even though Zakharov's strong turbulence theory continues to be investigated by many researchers (see the reviews by Goldman 1984 andRobinson 1997), the theory remains controversial to this date, and various numerical simulations and experiments to confirm the theory are inconclusive (Robinson and Newman 1990;Vyacheslavov et al 2002;Erofeev 2002). …”
Section: A Brief History Of Langmuir Turbulencementioning
confidence: 99%
“…11 The concept of turbulence spectra and energy flux distributed with respect to the spectra is fundamental. The wide-ranging interest in the turbulence spectra is not only motivated by the desire to gain a deeper understanding of SLT, but also because the spectra of the plasmons are believed to play a role in the turbulence acceleration by strong Langmuir plasmons.…”
Section: Plasmon Turbulence Spectra With the Filamentation Patterns Imentioning
confidence: 99%