Oblique propagation of ion acoustic soliton-cnoidal waves in a magnetized electron-positron-ion plasma with superthermal electrons

2014 ◽  
Vol 21 (3) ◽  
pp. 032111 ◽  
Author(s):  
Jian-Yong Wang ◽  
Xue-Ping Cheng ◽  
Xiao-Yan Tang ◽  
Jian-Rong Yang ◽  
Bo Ren
2021 ◽  
Vol 23 (3) ◽  
pp. 035301
Author(s):  
Muhammad KHALID ◽  
Ghufran ULLAH ◽  
Mohsin KHAN ◽  
Sheraz AHMAD ◽  
Sardar NABI ◽  
...  

Open Physics ◽  
2018 ◽  
Vol 16 (1) ◽  
pp. 563-567 ◽  
Author(s):  
Jianyong Wang ◽  
Ying Zeng ◽  
Zufeng Liang ◽  
Yani Xu ◽  
Yuanxiang Zhang

Abstract In this work, we are concerned with the ion acoustic quasi-soliton in an electron-positron-ion plasma with superthermal electrons and positrons. By using the reductive perturbation method, the Korteweg-de Vries equation is derived from the governing equations of ion acoustic waves. An interesting soliton-cnoidal wave solution of the Korteweg-de Vries equation and its quasi-soliton behaviour are presented. The influence of electron superthermality, positron superthermality and positron concentration ratio on characteristics of the quasi-soliton is confirmed to be significant.


2010 ◽  
Vol 374 (31-32) ◽  
pp. 3216-3219 ◽  
Author(s):  
E.I. El-Awady ◽  
S.A. El-Tantawy ◽  
W.M. Moslem ◽  
P.K. Shukla

2010 ◽  
Vol 17 (12) ◽  
pp. 122314 ◽  
Author(s):  
Prasanta Chatterjee ◽  
Uday narayan Ghosh ◽  
Kaushik Roy ◽  
S. V. Muniandy ◽  
C. S. Wong ◽  
...  

2009 ◽  
Vol 87 (8) ◽  
pp. 861-866 ◽  
Author(s):  
Tarsem Singh Gill ◽  
Amandeep Singh Bains ◽  
Narsehpal Singh Saini

A theoretical investigation was made for the ion acoustic wave in a weakly relativistic magnetized electron-positron-ion warm plasma. A Korteweg-de vries equation (KdV) is derived by using a standard reductive perturbation method. It is found that the presence of ion temperature (σ), ratios of positron-to-electron density (β), electron-to-positron temperature (α), and relativistic factor (Ur) significantly modify solitonic behavior. The authors observed that these parameters considerably change the amplitude and width of the solitary wave.


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