Effect of the dark soliton crystal temperature on the deflection of the bright soliton in a separate bright–dark screening soliton pair

Optik ◽  
2008 ◽  
Vol 119 (7) ◽  
pp. 303-308 ◽  
Author(s):  
Zhang Guangyong ◽  
Liu Jinsong ◽  
Wang Cheng ◽  
Zhang Huilan ◽  
Liu Shixiong
Applied laser ◽  
2011 ◽  
Vol 31 (5) ◽  
pp. 428-432
Author(s):  
吉选芒 Ji Xuanmang ◽  
姚纪欢 Yao Jihuan ◽  
刘劲松 Liu Jinsong

2021 ◽  
pp. 2150484
Author(s):  
Asif Yokuş

In this study, the auxiliary equation method is applied successfully to the Lonngren wave equation. Bright soliton, bright–dark soliton solutions are produced, which play an important role in the distribution and distribution of electric charge. In the conclusion and discussion section, the effect of nonlinearity term on wave behavior in bright soliton traveling wave solution is examined. The advantages and disadvantages of the method are discussed. While graphs representing the stationary wave are obtained, special values are given to the constants in the solutions. These graphs are presented as 3D, 2D and contour.


2017 ◽  
Vol 72 (11) ◽  
pp. 1053-1070 ◽  
Author(s):  
Tao Xu ◽  
Yong Chen

AbstractWe construct the Lax pair and Darboux transformation for the three-component coupled Hirota equations including higher-order effects such as third-order dispersion, self-steepening, and stimulated Raman scattering. A special vector solution of the Lax pair with 4×4 matrices for the three-component Hirota system is elaborately generated, based on this vector solution, various types of mixed higher-order localised waves are derived through the generalised Darboux transformation. Instead of considering various arrangements of the three potential functions q1, q2, and q3, here, the same combination is considered as the same type solution. The first- and second-order localised waves are mainly discussed in six mixed types: (1) the hybrid solutions degenerate to the rational ones and three components are all rogue waves; (2) two components are hybrid solutions between rogue wave (RW) and breather (RW+breather), and one component is interactional solution between RW and dark soliton (RW+dark soliton); (3) two components are RW+dark soliton, and one component is RW+bright soliton; (4) two components are RW+breather, and one component is RW+bright soliton; (5) two components are RW+dark soliton, and one component is RW+bright soliton; (6) three components are all RW+breather. Moreover, these nonlinear localised waves merge with each other by increasing the absolute values of two free parameters α, β. These results further uncover some striking dynamic structures in the multicomponent coupled system.


2007 ◽  
Vol 52 (6) ◽  
pp. 725-731 ◽  
Author(s):  
GuangYong Zhang ◽  
JinSong Liu ◽  
HuiLan Zhang ◽  
Cheng Wang ◽  
ShiXiong Liu

2010 ◽  
Vol 19 (02) ◽  
pp. 371-378 ◽  
Author(s):  
P. YOUPLAO ◽  
T. PHATTARAWORAMET ◽  
S. MITATHA ◽  
C. TEEKA ◽  
P. P. YUPAPIN

We propose a novel system of an optical trapping tool using a dark-bright soliton pulse-propagating within an add/drop optical filter. The multiplexing signals with different wavelengths of the dark soliton are controlled and amplified within the system. The dynamic behavior of dark bright soliton interaction is analyzed and described. The storage signal is controlled and tuned to be an optical probe which can be configured as the optical tweezer. The optical tweezer storage is embedded within the add/drop optical filter system. By using some suitable parameters, we found that the tweezers storage time of 1.2 ns is achieved. Therefore, the generated optical tweezers can be stored and amplified within the design system. In application, the optical tweezers can be stored and trapped light/atom, which can be transmitted and recovered by using the proposed system.


2020 ◽  
Vol 29 (6) ◽  
pp. 064212
Author(s):  
Zhen Liu ◽  
Wei-Guo Jia ◽  
Hong-Yu Wang ◽  
Yang Wang ◽  
Neimule Men-Ke ◽  
...  

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