摘要
强激光与等离子体之间相互作用,能够产生各种参量不稳定性过程和非线性效应。利用Karpman方法推导出横场包络所满足的非线性控制性方程,在一维情况下,获得孤波解。对孤波解进行分析,发现波包孤子的半宽反比于振幅;分析磁化等离子体中各参量对孤波半宽的影响。结果表明,在右旋圆偏振激光情况下,随着电子数密度的增大,孤波的半宽逐渐减小,而当磁场强度增大时,孤波的半宽逐渐增大;在左旋圆偏振激光情况下,随着电子数密度的增大,孤波的半宽逐渐增大,而当磁场强度增大时,孤波的半宽逐渐减小。
The interaction between intense laser and plasma can produce various parametric instability processes and nonlinear effects.In this paper,the nonlinear equation satisfied by the transverse field envelope is derived by Karpman method,and the solitary wave solution is obtained in one-dimensional case.It is found that the half width of the solitary wave is inversely proportional to the amplitude of the laser beam.The influence of various parameters in magnetized plasma on the half width of the solitary wave is analyzed.The results show that for the case of right-hand circularly polarized laser,the half width of soliton decreases with the increase of electron number density,and increases with the increase of magnetic field intensity.In the case of left-hand circularly polarized laser,the half width of soliton increases with the increase of electron number density,and decreases with the increase of magnetic field intensity.
作者
段杭杭
陈华英
刘三秋
Duan Hanghang;Chen Huaying;Liu Sanqiu(Department of Physics,College of Science,Nanchang University,Nanchang 330031,China)
出处
《强激光与粒子束》
CAS
CSCD
北大核心
2022年第2期19-25,共7页
High Power Laser and Particle Beams
基金
江西省聚变能与信息控制重点实验室基金项目(20171BCD40005)。
关键词
磁化等离子体
孤波
右旋圆偏振激光
左旋圆偏振激光
magnetized plasma
solitary wave
right-hand circularly polarized laser
left-hand circularly polarized laser