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M.?Ma?ek K.?Rohlena 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2010,56(1):79-90
The electron phase space evolution in a non-relativistic
and homogeneous laser plasma generated by a nanosecond laser in a
near infrared region in the presence of stimulated Raman scattering
is investigated by a numerical simulation. The mechanism of electron
acceleration in the potential wells of the plasma wave accompanying
the Raman back-scattering is analyzed in a 1D Vlasov-Maxwell model.
The dominant wave modes are both the backward and the forward
propagating Raman waves, each accompanied by a daughter
electrostatic wave. In addition to a strong interaction of plasma
electrons with the primary electrostatic wave in the case of
back-scattering, a cascading is observed consisting in a secondary
scattering of the primary Raman back-scattered wave. This phenomenon
reduces the Raman reflectivity and causes an acceleration of
electrons against the direction of the heating laser beam. Moreover,
the strong trapping in the primary electrostatic wave generated by
the Raman back-scattering leads due to the trapped particle
instability to a significant spectral broadening of the original
plasma wave and a subsequent intermittent behaviour of the
scattering process. The high phase velocity electrostatic daughter
wave of the forward Raman scattering cannot trap the electrons
directly, but there is an indication of non-resonant quasi-modes
combined of this wave and of the simultaneously existing
electrostatic daughter wave accompanying the Raman back-scattering.
The transform method is used for a solution of the set of partial
differential equations, which consists of the Vlasov equation and of
the full set of Maxwell equations in a 1D approximation. A
simplified Fokker-Planck collision term is added to overcome the
numerical instabilities during the simulation. The model has
relevance to a long scale plasma geometry, such as occurring in the
indirect drive experiments near the light entrance holes of target
hohlraum. 相似文献
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Optical seeding of plasma waves and the injection of electrons are key issues in self-modulated laser-wakefield accelerators. By implementing a copropagating laser prepulse with proper timing, we are able to control the growth of Raman forward scattering and the production of accelerated electrons. The dependence of the Raman intensity on prepulse timing indicates that the seeding of Raman forward scattering is dominated by the ionization-induced wakefield, and the dependence of the divergence and number of accelerated electrons further reveals that the stimulated Raman backward scattering of the prepulse plays the essential role of injecting hot electrons into the fast plasma wave driven by the main pulse. 相似文献
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Alain Ghizzo Daniele Del Sarto 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2014,68(10):1-10
The influence of low-frequency waves of kinetic nature induced by electron trapping in backward Stimulated Raman Scattering (SRS) is investigated. Semi-lagrangian Vlasov-Maxwell simulations are carried out not only for periodic boundary conditions but also in the case of an open plasma with parabolic shape, in optical mixing. We provide a numerical example of generation of KEEN (kinetic electrostatic electron nonlinear) waves nonlinearly induced from the SRS through a mechanism we first here elucidate. In particular we identify a process of backward scattering of the SRS probe light from the so generated KEEN waves, which may provide a mechanism for the possible experimental observation and measurement of such nonlinear structures. 相似文献
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The mechanism of electron acceleration in the stimulated Raman forward scattering of a monochromatic laser wave in a cold
plasma is investigated theoretically. It is shown that as a result of the stochastic interaction of the electrons with the
ponderomotive wave and with plasma waves excited in the scattering process, some of the electrons are accelerated to relativistic
energies.
Zh. Tekh. Fiz. 69, 3–8 (January 1999) 相似文献
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由于部分离化激光等离子体中存在束缚电子,它可显著改变其参量不稳定性。本文分析了部分离化激光等离子体的受激喇曼散射的非线性色散关系,计算了钕玻璃倍频和三倍频激光受激喇曼散射的增长率,结果表明,前向受激喇曼散射显著增强,后向受激喇曼散射影响不大。 相似文献
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A one-dimensional electrostatic particle-in-cell simulation is performed to study electrostatic wave excitation due to an electron beam in a plasma system. The excited fundamental and harmonic waves are analyzed with the fast Fourier transformation and the wavelet transformation. The second harmonic is suggested to be generated by wave-wave coupling during the nonlinear evolution, which involves forward propagating and backward propagating Langmuir waves. Furthermore, the background electrons may be heated and accelerated by the electrostatic waves. 相似文献
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The processes of nonlinear interaction of two high-power pump waves with widely spaced frequencies are studied in an optical fiber. Substantially increased output power of the Stokes components, generated via stimulated Raman scattering or stimulated four-wave mixing by one of the pump waves have been obtained in the field of the other pump wave and its Stokes components. For the first time the possibility to excited new spectral lines in the spectrum of one of the pump waves with frequency shifts characteristic for the other one, is experimentally demonstrated. 相似文献
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We present theoretical and numerical studies of the nonlinear interactions between intense electromagnetic waves in plasmas
containing high-and low-energy electron components. Such plasmas are frequently observed in laser-plasma experiments, where
the hot electron component is created by the acceleration of electrons by strong electrostatic waves that are created by the
laser-induced Raman forward and backward instabilities. The two-component electron plasma is described by the Vlasov equation
for the hot electrons and the hydrodynamic equations for the cold electrons, which are coupled nonlinearly to the electromagnetic
wave equation and the Poisson equation for the potential. The present nonlinear system is shown to admit electromagnetic solitary
waves correlated with a positive potential and trapped electron islands from the hot electron population.
The text was submitted by the authors in English. 相似文献
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在相干反斯托克斯拉曼散射(coherent anti-Stokes Raman scattering,CARS)显微镜中,共线传输的紧聚焦高斯光束激发具有不同形状和尺寸的待测样品所产生的CARS信号场的空间分布决定了整体系统的结构特点.建立了紧聚焦条件下球形样品产生CARS信号场的理论模型.利用矢量波动方程分析了紧聚焦条件下线偏振的高斯光束的光场强度和相位分布.利用格林函数求解该模型中CARS信号场的矢量波动方程,模拟计算得到了不同直径球形样品的远场CARS信号场的空间分布.理论分析和模拟计算结果表明,对于小体积的球形样品,前向和背向传输的CARS信号场强度接近,因此采用大数值孔径物镜背向探测方式即可获得高对比度图像.对于大体积球形样品,CARS信号场的强度大幅增强,且发射方向主要集中在前向的一定立体角内.因此,采用小数值孔径物镜即可有效收集前向传输的CARS信号. 相似文献
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A. A. Andreev V. G. Bespalov E. V. Ermolaeva R. R. E. Salomaa 《Optics and Spectroscopy》2007,102(1):98-105
The potential for time compression of ultraintense laser pulses in plasma based on nonlinear interactions between waves during backward stimulated Raman scattering is analyzed analytically and numerically. The optimal conditions for obtaining a maximal energy conversion coefficient of 10-ps laser pulses to the energy of 100-fs Stokes pulses are found. 相似文献
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S. A. Dvinin D. K. Solikhov Sh. S. Nurulkhakov 《Moscow University Physics Bulletin》2017,72(4):345-350
Brillouin scattering in an infinite medium is anisotropic, in this case the threshold of absolute instability is caused by attenuation of scattered waves. If the collision attenuation mechanism prevails, the minimum threshold value is observed during backward scattering. For a scattering region limited in the longitudinal direction (parallel to the direction of pumping wave propagation), the backward scattering threshold will be greater than for an infinite medium due to convective loss associated with energy removal by scattered waves. In this paper, the scattering of a wide wave beam in plasma is considered, whose dimension in the transverse direction to the pumping wave propagation substantially exceeds the dimension in the longitudinal direction. It was revealed that in this case, during angle scattering the instability threshold can be less than the threshold for backward scattering due to the increased time of radiation removal from the interaction region. This effect was not taken into account previously. In turn, the decrease of the threshold leads to increasing the radiation loss, which is important in plasma heating problems. The results can also be used for plasma diagnostics. 相似文献
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We investigate the nonlinear evolution of the backward stimulated Raman scattering (BSRS) in the regime where the nonlinear saturation mechanism is the Langmuir decay instability resulting from the coupling of the BSRS-generated Langmuir wave with the ion acoustic waves. We present numerical results obtained with a fluid-type code in one- and two-dimensional spatial dimensions, in the case of an inhomogeneous plasma. The plasma density is under quarter-critical and depends linearly on the longitudinal spatial coordinate, in the regime where the Rosenbluth gain factor for the amplitude, denoted as G(Ros), is in the range pi/2< or =G_(Ros)< or =6. We observe that the Langmuir decay instability is able to suppress the gradient stabilization and restore the absolute nature of BSRS, thus leading to a significantly increased BSRS reflectivity. 相似文献
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非线性拉曼激光雷达测量CO2气体的研究 总被引:2,自引:2,他引:0
提出了利用气体的受激拉曼散射(SRS)效应激光雷达光源来探测大气中的CO2气体的新方法,设计出探测大气中CO2气体含量的非线性拉曼增益激光雷达,用Nd:YAG激光器(1064 nm)的三倍频光(354.7 nm)通过分别装有CO2气体和N2气体的拉曼管,分别得到CO2气体和N2气体的受激拉曼散射的一阶斯托克斯线(S1),并用S1线作为雷达的种子发射光源.通过实验得到拉曼管中的气压与S1能量的变化关系,对其优化条件和物理机制进行了分析.该实验方法已经成功测出了大气中CO2气体的回波电压信号. 相似文献
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Depierreux S Labaune C Fuchs J Pesme D Tikhonchuk VT Baldis HA 《Physical review letters》2002,89(4):045001
Thomson scattering has been used to investigate the nonlinear evolution of electron plasma waves (EPWs) generated by stimulated Raman scattering (SRS). Two complementary diagnostics demonstrate the occurrence of the cascade of Langmuir decay instabilities (LDI). The EPW wave-number spectrum displays an asymmetric broadening towards small wave numbers, interpreted as a signature of the secondary EPWs produced in the LDI cascade. The number of cascade steps is in agreement with the broadening of the associated ion-acoustic-waves' spectra. The total energy transferred in the EPWs cascade is found to be either less than or of the same order of magnitude as the energy of the primary EPW. 相似文献
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左手系材料界面上的非线性TE电磁波 总被引:4,自引:4,他引:0
针对电磁波在非线性左手系材料中的传播性质, 分别研究了左、右手系材料界面以及两左手系材料界面上非线性TE表面波的传播行为讨论了导波的频率特性、色散关系以及群速度随频率的变化规律分析表明,两种界面上的非线性TE表面波均存在频率通带和禁带,且带宽是传播功率的函数揭示了在一定条件下,左、右手系材料界面上既可以支持正向传播的非线性TE表面波,也可以支持反向传播的非线性TE表面波;两左手系材料界面上表面波的传播性质因材料参量的变化差异较大,一定参量条件下,该界面上仅支持反向传播的非线性TE表面波. 相似文献
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The propagation of light waves in an underdense plasma is studied using one-dimensional Vlasov-Maxwell numerical simulation.It is found that the light waves can be scattered by electron plasma waves as well as other heavily and weakly damping electron wave modes,corresponding to stimulated Raman and Brilluoin-like scatterings.The stimulated electron acoustic wave scattering is also observed as a high scattering level.High frequency plasma wave scattering is also observed.These electron electrostatic wave modes are due to a non-thermal electron distribution produced by the wave-particle interactions.The collision effects on stimulated electron acoustic wave and the laser intensity effects on the scattering spectra are also investigated. 相似文献
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多脉冲激光尾波场加速电子方法中限制尾波场振幅的主要机理是“相位失谐”,起源于非线 性效应导致尾波波长随振幅的增长而变大,从而后续脉冲逐渐偏离加速相位. 借助2D3V PIC 模拟方法优化各脉冲之间的间距,使之等于前面脉冲激发的尾波波长,模拟结果表明激发了 更大振幅的尾波场,同时激发了更强的“前向Raman散射”,它在限制尾波场进一步增长的 过程发挥了重要作用.
关键词:
多脉冲激光尾波加速
有质动力
相位失谐
前向Raman散射 相似文献