Erratum: “Finite amplitude envelope solitons in a pair-ion plasma” [Phys. Plasmas 14, 032107 (2007)]

2007 ◽  
Vol 14 (10) ◽  
pp. 109902
Author(s):  
W. M. Moslem ◽  
I. Kourakis ◽  
P. K. Shukla
2007 ◽  
Vol 14 (3) ◽  
pp. 032107 ◽  
Author(s):  
W. M. Moslem ◽  
I. Kourakis ◽  
P. K. Shukla

1987 ◽  
Vol 35 (10) ◽  
pp. 4273-4279 ◽  
Author(s):  
R. Blaha ◽  
E. W. Laedke ◽  
K. H. Spatschek

1977 ◽  
Vol 20 (8) ◽  
pp. 1286 ◽  
Author(s):  
H. Schamel ◽  
M. Y. Yu ◽  
P. K. Shukla

Author(s):  
Himangshu Sahoo ◽  
Chinmay Das ◽  
Swarniv Chandra ◽  
Basudev Ghosh ◽  
Kalyan Kumar Mondal

1993 ◽  
Vol 252 ◽  
pp. 703-711 ◽  
Author(s):  
Michael S. Longuet-Higgins

The existence of steady solitary waves on deep water was suggested on physical grounds by Longuet-Higgins (1988) and later confirmed by numerical computation (Longuet-Higgins 1989; Vanden-Broeck & Dias 1992). Their numerical methods are accurate only for waves of finite amplitude. In this paper we show that solitary capillary-gravity waves of small amplitude are in fact a special case of envelope solitons, namely those having a carrier wave of length 2π(T/ρg)1½2 (g = gravity, T = surface tension, ρ = density). The dispersion relation $c^2 = 2(1-\frac{11}{32}\alpha^2_{\max)$ between the speed c and the maximum surface slope αmax is derived from the nonlinear Schrödinger equation for deep-water solitons (Djordjevik & Redekopp 1977) and is found to provide a good asymptote for the numerical calculations.


2009 ◽  
Vol 16 (6) ◽  
pp. 062305 ◽  
Author(s):  
Nusrat Jehan ◽  
M. Salahuddin ◽  
Arshad M. Mirza

2011 ◽  
Vol 18 (8) ◽  
pp. 084702 ◽  
Author(s):  
Yan-Xia Xu ◽  
Zong-Ming Liu ◽  
Mai-Mai Lin ◽  
Yu-Ren Shi ◽  
Wen-Shan Duan

2014 ◽  
Vol 21 (8) ◽  
pp. 082105
Author(s):  
Hong-E Du ◽  
Li-Hong Cheng ◽  
Zi-Fa Yu ◽  
Ju-Kui Xue

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