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Effect of Magnetic Field and Plasma Density on Nonlinear Solitary Waves in a Relativistic Plasma

机译:磁场和等离子体密度在相对论等离子体中非线性孤立波的影响

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Modified Korteweg-deVries (mK-dV) equation is derived for perturbed potential and solved in order to study the potential structure for the propagation of nonlinear solitary waves (solitons) in a magnetized spatially inhomogeneous plasma having relativistic ions and electrons. It is found that fast and slow modes occur in the plasma and only the fast modes correspond to the solitons. Solitons are possible for a particular range of wave-propagation angle θ (angle between wave vector and direction of the magnetic field) governed by mass ratio (m_i/m_e), temperature ratio (T_i/T_e) and relativistic speeds of ions and electrons. Effect of magnetic field is to decrease the soliton width and energy. The amplitude and energy of soliton get lower and the width gets wider when it propagates into higher plasma density region. The waves propagating at larger angles with the direction of magnetic field correspond to the solitons of higher amplitude and smaller width.
机译:改进的Korteg-Devries(MK-DV)方程被衍生出扰动电位并解决,以研究具有相对定义离子和电子的磁化空间不均匀等离子体中的非线性孤立波(孤子)的潜在结构。发现在等离子体中发生快速和慢速模式,并且仅快速模式对应于孤子。由质量比(M_I / M_E),温度比(T_I / T_E)和离子和电子的相对速度来控制的特定波传播角θ(波矢量和磁场方向之间的角度之间的角度之间的角度传播角度θ(波矢量和方向之间的角度)可以进行孤子。磁场的效果是降低孤子宽度和能量。孤子的幅度和能量越来越低,并且当它传播到更高的等离子体密度区域时宽度越宽。在磁场方向上以较大角度传播的波对应于较高幅度和较小宽度的孤子。

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