模拟 ps激光驱动的类氖锗19.6 nm X光激光

 瞬态电子碰撞激发产生X光激光的机制可以极大减少X光激光的泵浦能量。模拟了脉宽为1 ps,波长1.053 μm的钕玻璃激光驱动的类氖锗X光激光。模拟表明,在临界面附近可以产生高达60 cm ^-1的增益,还计算了X光激光在等离子体中的传播,计算表明X光激光在等离子体中的折射效应仍然是影响X光激光输出强度及分布的重要因素。     

改进型双盘靶实验与分析

 采用改进型双盘靶结构,初级改用为斜柱腔结构,激光加热初级薄箔,后向出射的X光烧蚀次级,这样降低初级等离子体喷射的影响,使烧蚀次级的X光更纯净。采用X光条纹相机测量双盘靶等离子体喷射的时空扫描图象,采用两台软X光谱仪分别对初级和次级辐射的X光进行测量,研究次级盘对初级发射的X光谱的改造。测量结果表明：这种结构的双盘靶基本上能避免初级盘喷射等离子体的影响,初级盘后向辐射的X光谱具有明显 的N和O带谱结构,而次级辐射的X光谱主要以O带为主。     

小孔等离子体运动实验方法

在间接驱动惯性约束聚变的黑腔中,辐射烧蚀的高Z等离子体的流体力学运动过程对激光注入黑腔的效率、辐射场均匀性和通过诊断口的黑腔辐射温度诊断都有显著影响。为研究诊断口在黑腔辐射场中的等离子体缩口过程,用激光产生X光辐射加热低Z泡沫填充的金黑腔诊断口,以激光辐照钛平面靶产生的2～5 keV高能段窄能区X光作为背光源,用X光分幅相机获得了源靶和小孔靶两种靶型的小孔等离子体运动过程图像,研究了X光烧蚀的小孔等离子体的流体力学运动过程,探索了定量测量小孔等离子体面密度的空间分布与时间演化过程的实验诊断方法,初步给出小孔等离子体的面密度。     

激光线聚焦产生的等离子体特性

一、引言随着激光产生的线状等离子体作为增益介质的X射线激光研究得到初步成功并为今后真正高强度相干X射线激光输出作准备。近几年来,利用各种探测工具对线状等离子体介质特性开展了广泛的研究。文献[1]利用光探针专门对不同时刻(50-500ps)下的等离子体性质进行诊断,发现等离子体在膨胀时,会出现许多细丝结构且这种结构随时间推移而更加显著。又从X光针孔像中发现激光等离子体的X射线(LPX)发射区也极不均匀。在文献[2]的实验     

快速响应的超软X光探测器

核聚变等离子体的各种辐射,携有大量等离子体信息。探测这些辐射,是研究等离子体的重要课题之一。在激光等离子体研究中,驱动源的脉宽为毫微秒和亚毫微秒量级,要求探测的仪器时间响应极快速。为了得到激光等离子体电子温度、密度等信息,我们对等离子体辐射的X光连续谱进行了探测研究,并研制出多道X光连续谱仪。     

0.35μm激光辐照下柱腔靶的等离子体状态与运动特性

 使用针孔相机配X光条纹相机、法拉第杯等观测了腔靶等离子体的运动特性、腔内壁衬CH膜对高Z高密度等离子体运动的抑制现象以及隔离膜对等离子体膨胀的影响。并用硬X光能谱法和受激喇曼散射光的短波截止推算了相应的腔内热等离子体电子温度。 这些结果有助于0.35μｍ激光辐照下腔靶辐射场特性的深入研究以及未来神光Ⅱ腔靶构型的设计。     

托卡马克等离子体不同平衡位形下的电子回旋波电流驱动

在给定的等离子体总电流和中心电流密度条件下,数值求解平衡方程,求出不同拉长比和三角形变因子的托卡马克等离子体温度、密度、磁场分布,然后通过求解波迹方程和Fokker-Planck方程,分别计算这些位形下的电子回旋波波迹和电流驱动.结果表明：电子回旋波X模从顶部发射时,随着拉长比的增大,波迹会向弱场侧偏移.电子回旋波X模从弱场侧发射时,电子回旋波在等离子体中传播沉积的功率份额随着拉长比的增大而增加,驱动电流位置随着三角形变因子的增大向等离子体中心移动.驱动电流位置随环向和极向发射角的减小向中心移动,对应的电流密度峰值也变大.     

辐射烧蚀铝箔数值模拟研究

 利用一维多群辐射输运程序RDMG数值模拟神光II条件下辐射烧蚀铝箔的实验研究,详细描述了X光在铝箔中的辐射输运过程,清楚地显示了辐射热波在铝箔中的传播,给出铝等离子体温度密度的时空分布、铝箔背面出射的X光能谱及出射X光各能区能流随时间的变化,分析出射X光的能区对测量结果的影响,对神光II条件下辐射烧蚀铝箔的厚度范围进行初步的探讨。数值结果与实验结果相吻合。     

周期量级超短激光脉冲在近临界密度等离子体中形成的光孤子

利用一维粒子模拟程序，观测到周期量级的超短激光脉冲在等离子体中可以以孤子形式传播.它在一定密度等离子体中以较高的群速度向前传播，并在到达等离子体与真空界面时发生反射和透射.当入射激光脉冲强度增大时，非线性调制效应使它产生较大的频率下移，致使光孤子传播速度变小.另外，对于同样光强下的几十个周期以上的光脉冲，它在等离子体中传播时形成的则是一连串低频的被捕获在等离子体中的光孤子. 关键词： 光孤子 超短激光脉冲 等离子体 粒子模拟     

提高X光激光相干性的镶嵌靶的研究

 在以锗等离子体为增益介质的X光激光实验研究中，使用铜锗镶嵌靶可以获得一维横向宽度很窄的柱状等离子体，这有利于X光激光的单横模输出。本文对铜锗镶嵌靶进行了实验研究。     

K-P-Burgers equation in negative ion-rich relativistic dusty plasma including the effect of kinematic viscosity

The stationary solution is obtained for the K–P–Burgers equation that describes the nonlinear propagations of dust ion acoustic waves in a multi-component, collisionless, un-magnetized relativistic dusty plasma consisting of electrons, positive and negative ions in the presence of charged massive dust grains. Here, the Kadomtsev–Petviashvili(K–P) equation, threedimensional(3D) Burgers equation, and K–P–Burgers equations are derived by using the reductive perturbation method including the effects of viscosity of plasma fluid, thermal energy, ion density, and ion temperature on the structure of a dust ion acoustic shock wave(DIASW). The K–P equation predictes the existences of stationary small amplitude solitary wave,whereas the K–P–Burgers equation in the weakly relativistic regime describes the evolution of shock-like structures in such a multi-ion dusty plasma.     

Low frequency electrostatic nonlinear structures in an inhomogeneous magnetized non-Maxwellian electron–positron–ion plasma

The properties of low frequency (coupled acoustic and drift wave) nonlinear structures including solitary waves and double layers in an inhomogeneous magnetized electron–positron–ion (EPI) nonthermal plasma with density and temperature inhomogeneities are studied in a simplified way. The nonlinear differential equation derived here for the study of double layers in the inhomogeneous EPI plasma resembles with the modified KdV equation in the stationary frame. But the method used for the derivation of nonlinear differential equation is simple and consistent to give both the stationary solitary waves and double layers. Further, the illustrations show that superthermality κ, drift velocity and temperature inhomogeneity have significant effects on the amplitude, width, and existence range of the structures.     

Ion-Acoustic Solitary Waves in Multicomponent Plasmas with Negative Ions

By using the perturbation technique, a Kortewege-de-Vries (K-dV) equation for a multicomponent plasma with negative ions and isothermal electrons has been derived. We have discussed the stationary solutions of K-dV equation and it has shown that in the presece of multiple ions, the amplitude of solitons exhibits interesting behaviour, especiallY when the negative ions are present.     

Effect of beam-plasma interaction on ion transport through a cyclotron injector

The influence of collective effects associated with transverse plasma oscillations excited by a beam of negative ions on the neutralization of the space charge due to fast ions is studied. Conditions for the dynamic deneutralization of an unstable ion beam are refined. Analytic expressions for the plasma ion density distribution and for the stationary electric field in a partially neutralized beam are obtained. The equation of motion of a beam in the self-electric field and in an external magnetic field is used to determine the effect of secondary charged particles on the transport of negative ions through the injector of a cyclotron.     

Bragg Effects in Microwave Transmission through Stationary Plasma Structures

We describe the first of a series of experiments designed to study, in a double-plasma (DP) device (3-cm) microwave Bragg scattering from stationary plasma structures, and from systems of plasma waves and "irregularities." This paper deals with Bragg effects in microwave transmission through stationary plasma density structures, consisting of a) a cylindrical plasma column, b) a single plasma slab, and c) a rotatable system of multiple equally spaced plasma slabs.     

Solitons in collisionless cold plasma

The relativistic nonlinear self-consistent equations for a collisionless plasma with stationary ions are transformed into a form appropriate for finding exact analytic solutions. It is shown that for an axial system with planar geometry, the two-dimensional stationary equations for this system can be reduced to the sh-Gordon equation. The exact solution of this equation describing the charge-density equilibrium configuration is obtained, the solution having sharp transverse boundaries and a soliton form in longitudinal direction. The generalization to the nonstationary case is considered in an perturbative approach.     

托卡马克中低杂电流驱动对不稳定性的影响

本文求解了稳定情形下的准线性动力方程，并计算了等离子体中异常多卜勒共振所激发的倾斜模的增长率或衰减率与低杂波能密度的关系，文中比较了感应电场相对于低杂电流驱动方向取正反两个方向的情形。     

Diffraction of high-intensity field in focal region as dynamics of nonlinear system with low-frequency dispersion

The stationary profile in the focal region of a focused nonlinear acoustic wave is described. Three models following from the Khokhlov-Zabolotskaya (KZ) equation with three independent variables are used: (i) the simplified one-dimensional Ostrovsky-Vakhnenko equation, (ii) the system of equations for paraxial series expansion of the acoustic field in powers of transverse coordinates, and (iii) the KZ equation reduced to two independent variables. The structure of the last equation is analogous to the Westervelt equation. Linearization through the Legendre transformation and reduction to the well-studied Euler-Tricomi equation is shown. At high intensities the stationary profiles are periodic sequences of arc sections having singularities of derivative in their matching points. The occurrence of arc profiles was pointed out by Makov. These appear in different nonlinear systems with low-frequency dispersion. Profiles containing discontinuities (shock fronts) change their form while passing through the focal region and are non-stationary waves. The numerical estimations of maximum pressure and intensity in the focus agree with computer calculations and experimental measurements.

     

Analysis of the evolution of perturbations in a magnetized collisionless plasma with an integral-equation technique

Summary A technique recently proposed to study the classical problem of the evolution of small perturbations in a collisionless unmagnetized plasma is extended to a magnetized plasma. A time-convolutive integral equation for the plasma density is obtained from the Vlasov equation for a homogeneous plasma in a uniform, stationary magnetic field. The equation can be solved by means of simple numerical algorithms and, in some cases, analytical solutions can be obtained. The procedure proves to be analytically simpler than the classical one and is more convenient from a numerical point of view. Techniques of solution are presented and analytical and numerical results for electrostatic perturbations are discussed.