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Four-wave mixing and phase conjugation in plasmas.

机译:等离子体中的四波混合和相位共轭。

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摘要

Nonlinear optical effects such as Stimulated Brillouin Scattering, Stimulated Raman Scattering, self-focusing, wave-mixing, parametric mixing, etc., have a long history in plasma physics. Recently, four-wave mixing in plasmas and its applications to phase conjugation has been extensively studied. Although four-wave mixing (FWM), using various nonlinear mediums, has many practical applications in the visible regime, no successful attempt has been made to study or demonstrate FWM for wavelengths longer than 10{dollar}mu{dollar}m. Plasmas as phase conjugate mirrors have received considerable attention since they become more efficient at longer wavelengths (far-infrared to microwave). The purpose of this thesis is to study various fundamental issues which concern the suitability of plasmas for four-wave mixing and phase conjugation. The major contributions of this thesis are the identification and study of thermal and ionization nonlinearities as potential four-wave mixing and phase conjugation mechanisms and the study of the affect of density inhomogeneities on the FWM process.; Using a fluid description for the plasma, this thesis demonstrates that collisional heating generates a thermal force which substantially enhances the phase conjugate reflectivity. Numerical estimates of the phase conjugate reflectivity indicate that for modest power levels, gains {dollar}<{dollar}1 are possible in the submillimeter to centimeter wavelength range.; The prospect of using a novel ionization nonlinearity in weakly ionized plasmas for wave-mixing and phase conjugation is discussed. The ionization nonlinearity arises from localized heating of the plasma by the beat-wave. Wherever, the local temperature is increased, a plasma density grating is produced due to increased electron-impact ionization. Numerical estimates of the phase conjugate reflectivity indicate reflectivities in the range of 10{dollar}sp{lcub}-4{rcub}{dollar}-{dollar}10sp{lcub}-3{rcub}{dollar} are possible in a weakly ionized steady-state gas discharge plasma. Larger reflectivities may be possible for pulsed plasma sources.; Most of the literature concerning FWM and phase conjugation in plasmas has assumed that the plasmas are isotropic, homogeneous, and quiescent. Since plasmas seldom satisfy any of the above criteria, a more complete theory of FWM in the presence of plasma density fluctuations is necessary. One chapter in this thesis focus on the effects of density fluctuations (inhomogeneities) on the FWM process.
机译:非线性光学效应,如受激布里渊散射,受激拉曼散射,自聚焦,波混合,参量混合等,在等离子体物理学中具有悠久的历史。最近,对等离子体中的四波混合及其在相共轭中的应用进行了广泛的研究。尽管使用各种非线性介质的四波混频(FWM)在可见光范围内有许多实际应用,但尚未进行成功的尝试来研究或证明波长大于10微米的FWM。等离子作为相位共轭反射镜已经受到相当大的关注,因为它们在更长的波长(远红外到微波)下变得更有效率。本文的目的是研究与等离子体在四波混频和相位共轭中的适用性有关的各种基本问题。本论文的主要贡献是对热和电离非线性的识别和研究,作为潜在的四波混合和相位共轭机制,以及研究密度不均匀性对FWM过程的影响。使用对等离子体的流体描述,本论文证明了碰撞加热产生的热力实质上增强了相位共轭反射率。相位共轭反射率的数值估计表明,对于中等功率水平,在亚毫米至厘米波长范围内,增益{dollar} <{dollar} 1是可能的。讨论了在弱电离等离子体中使用新型电离非线性进行混波和相位共轭的前景。电离非线性是由拍波对等离子体的局部加热引起的。无论何时,局部温度升高,由于电子撞击电离的增加而产生等离子体密度光栅。对相位共轭反射率的数值估计表明,在弱的情况下,反射率可能在10 {dol}} {lcub} -4 {rcub} {dollar}-{dollar} 10sp {lcub} -3 {rcub} {dollar}的范围内电离的稳态气体放电等离子体。对于脉冲等离子体源,可能会有更大的反射率。关于FWM和等离子体中的相位共轭的大多数文献都假定等离子体是各向同性的,均质的和静态的。由于等离子体很少满足上述任何标准,因此在存在等离子体密度波动的情况下,需要更完整的FWM理论。本文的一章重点讨论了密度波动(不均匀性)对FWM过程的影响。

著录项

  • 作者

    Federici, John Francis.;

  • 作者单位

    Princeton University.;

  • 授予单位 Princeton University.;
  • 学科 Physics Fluid and Plasma.; Physics Optics.
  • 学位 Ph.D.
  • 年度 1989
  • 页码 195 p.
  • 总页数 195
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 等离子体物理学;光学;
  • 关键词

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