On the rogue waves propagation in non-Maxwellian complex space plasmas

被引:37
作者
El-Tantawy, S. A. [1 ]
El-Awady, E. I. [1 ]
Tribeche, M. [2 ]
机构
[1] Port Said Univ, Fac Sci, Dept Phys, Port Said 42521, Egypt
[2] Univ Bab Ezzouar, USTHB, Fac Phys, Plasma Phys Grp,Theoret Phys Lab, Algiers 16111, Algeria
关键词
ELECTROSTATIC SOLITARY STRUCTURES; ION-ACOUSTIC SOLITONS; FREAK WAVES; DOUBLE-LAYERS; ENERGY; FLOW;
D O I
10.1063/1.4935916
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The implications of the non-Maxwellian electron distributions (nonthermal/or suprathermal/or non-extensive distributions) are examined on the dust-ion acoustic (DIA) rogue/freak waves in a dusty warm plasma. Using a reductive perturbation technique, the basic set of fluid equations is reduced to a nonlinear Schrodinger equation. The latter is used to study the nonlinear evolution of modulationally unstable DIA wavepackets and to describe the rogue waves (RWs) propagation. Rogue waves are large-amplitude short-lived wave groups, routinely observed in space plasmas. The possible region for the rogue waves to exist is defined precisely for typical parameters of space plasmas. It is shown that the RWs strengthen for decreasing plasma nonthermality and increasing superthermality. For nonextensive electrons, the RWs amplitude exhibits a bit more complex behavior, depending on the entropic index q. Moreover, our numerical results reveal that the RWs exist with all values of the ion-to-electron temperature ratio sigma for nonthermal and superthermal distributions and there is no limitation for the freak waves to propagate in both two distributions in the present plasma system. But, for nonextensive electron distribution, the bright- and dark-type waves can propagate in this case, which means that there is a limitation for the existence of freak waves. Our systematic investigation should be useful in understanding the properties of DIA solitary waves that may occur in non-Maxwellian space plasmas. (C) 2015 AIP Publishing LLC.
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页数:6
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