简并量子等离子体中的量子电子-声学包络孤子及其调制不稳定性

Foisal B. T. Siddiki, Abdullah Al Mamun, M. Amin
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引用次数: 0

摘要

从理论上研究了简并量子等离子体(包含非相对论简并电子、超热或超分布电子和固定离子)中线性和非线性量子电子声(QEA)波的基本特征。采用约化微扰法推导了非线性Schödinger (NLS)方程。得到了NLS方程的平稳孤子解,并对其进行了解析和数值检验,从而确定了QEA包络孤子的基本特征。研究发现,冷电子的简并态和交换/玻姆势以及热电子的超热效应显著地改变了线性和非线性QEA波的基本性质。我们观察到,当k < kc时,QEA波是调制不稳定的,其中kc是QEA波数k的最大值(临界),低于k时,QEA波是调制不稳定的,并且当k < kc时,NLS方程的解产生明亮的包络孤子,它们被发现在空间(ξ)和时间(τ)轴上都是局域的。我们还观察到,随着谱指数κ的增加,波数的临界值(QEA包络亮孤子的振幅)减小(增大)。本研究结果对理解强激光、半导体器件、微电子器件等辐照金属产生的固体密度等离子体中的局部静电扰动具有重要意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum Electron-acoustic Envelope Solitons and Their Modulational Instability in a Degenerate Quantum Plasma
The basic features of linear and nonlinear quantum electron-acoustic (QEA) waves in a degenerate quantum plasma (containing non-relativistically degenerate electrons, superthermal or κ-distributed electrons, and stationary ions) are theoretically investigated. The nonlinear Schödinger (NLS) equation is derived by employing the reductive perturbation method. The stationary solitonic solution of the NLS equation is obtained, and examined analytically as well as numerically to identify the basic features of the QEA envelope solitons. It has been found that the effects of the degeneracy and exchange/Bohm potentials of cold electrons, and superthermality of hot electrons significantly modify the basic properties of linear and nonlinear QEA waves. It is observed that the QEA waves are modulationally unstable for k < kc, where kc is the maximum (critical) value of the QEA wave number k below which the QEA waves are modulationally unstable), and that for k < kc the solution of the NLS equation gives rise to the bright envelope solitons, which are found to be localized in both spatial (ξ) and time (τ) axes. It is also observed that as the spectral index κ is increased, the critical value of the wave number (amplitude of the QEA envelope bright solitons) decreases (increases). The implications of our results should be useful in understanding the localized electrostatic perturbation in solid density plasma produced by irradiating metals by intense laser, semiconductor devices, microelectronics, etc.
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