2015
DOI: 10.1002/ctpp.201500036
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Collisionless Damping of Geodesic Acoustic Mode in a Multi‐Ion Plasma with Superthermal Ions

Abstract: The dispersion relation of geodesic acoustic mode is investigated in a multi-ion toroidal plasma on the basis of linear gyrokinetic equations where ions are assumed to take a nonextensive distribution. It is found that the frequency of GAM becomes larger with the decrease of q. Consequently, GAM will damp more rapidly. The effective charge corresponding to the maximum damping rate is found to move towards unity as q decreases. As indicates that in a plasma with superthermal bulk ions, the influence of the impu… Show more

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Cited by 5 publications
(3 citation statements)
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“…The effects of Z eff in multi-ion species plasmas have also been investigated using linear GK equations and non-Maxwellian ion energy distributions [445]. Both the GAM frequency (linearly) and the damping rate (nonlinearly) were found to fall with increasing Z eff = j=b,i q 2 j n j / j=b,i q j n j , where b, i refer to bulk and impurity ion respectively, and the degree of non-Maxwellian-ness of the ion distribution function (e.g.…”
Section: Impurities and Effective Charge Z Effmentioning
confidence: 99%
“…The effects of Z eff in multi-ion species plasmas have also been investigated using linear GK equations and non-Maxwellian ion energy distributions [445]. Both the GAM frequency (linearly) and the damping rate (nonlinearly) were found to fall with increasing Z eff = j=b,i q 2 j n j / j=b,i q j n j , where b, i refer to bulk and impurity ion respectively, and the degree of non-Maxwellian-ness of the ion distribution function (e.g.…”
Section: Impurities and Effective Charge Z Effmentioning
confidence: 99%
“…It is important to note that the distribution function with q < 1, compared with the Maxwellian limits, there are more particles with the velocities faster than the thermal speed, which is called the super‐extensive case, whereas the distribution function with q > 1 depicts a large number of low‐speed particles, which is called the sub‐extensive case. This q ‐non‐extensive distribution has been successfully employed in plasma physics, such as plasma oscillations in a collisionless thermal plasma, the thermal dispersion relation in a collisionless plasmas, dust‐charging processes, dust ion acoustic waves or dust acoustic waves in a dusty plasma by taking non‐extensive electrons, non‐extensive ions, or both to be non‐extensive, and ion and positron acoustic solitons in magnetized dusty plasma . Recently, a great deal of attention has been paid to the Bohm criterion and the sheath structure in plasma with non‐extensively distributed electrons .…”
Section: Introductionmentioning
confidence: 99%
“…In particular, with the development of nonextensive statistics, when it is recognized that this new statistical theory can be used as a theoretical basis for the study of power-law distributed plasmas, the investigations of q-distributed plasmas are becoming increasingly widespread across both astrophysics and space science with an exponential growth rate of relevant publications (see the list of publications on plasma physics in Ref. [3]), which include a wide variety of waves and instabilities both in different electron-ion plasmas and dusty plasmas, solar wind and properties of other plasmas etc [20][21][22][23][24][25][26][27][28][29][30][31][32][33].…”
mentioning
confidence: 99%