闪烁x射线照相二极管中光束与等离子体和气体相互作用的数值模拟

I. V. Glazyrin, A. V. Karpeev, Y. Kandiev, O. G. Kotova, D. Modestov, V. Plokhoi, S. N. Shcherbakova, E.Yu. Smirnov
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摘要

只提供摘要形式。在射线照相用新型二极管的研制过程中,有许多问题需要解决。(1)在自磁致缩二极管中,电极附近的等离子体对电子束聚焦和轫致辐射形成有显著影响。(2)有必要了解电子束的角度扩展和初始旋转对聚焦特性的影响。(3)如果采用充气聚焦电池,其效果取决于气体密度的选择。为了回答上述问题,开发了PICNIC混合代码,它由几个相互关联的部分组成:计算相对论粒子(电子和离子)动力学的二维PIC代码,Maxwell方程的三维FDTD求解器,热电子和离子的二维MHD描述,定义碰撞后粒子动量和角度的蒙特卡罗代码PPJZMA。为了计算磁场,考虑了通过阳极表面的电流。生成器参数是下一个。对电压为5 MV、电流为30 kA的发电机的充气聚焦二极管进行了分析。对于自磁箝位二极管,发电机使用10.0 MV, 200 kA, 50 nsec的FWHM电脉冲。计算结果表明,二极管在不同的电流值下工作:最初在真空中准均匀的电子束运动,然后在等离子体中不稳定的大电流电子束运动。等离子体内部的回流电流和局部电流密度的大小在这些束等离子体相互作用的集体效应中起着重要的作用。这些过程在很大程度上取决于光束的初始参数、角速度和能量的扩散。对于棒捏二极管,轫致辐射产生过程中电子的入射角可在50度范围内变化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Numerical Simulation of Beam Interaction with Plasma and Gas in Diodes for Flash X-Ray Radiography
Summary form only given. A number of questions should be solved in the course of development of new diodes for radiographic applications. (1) In self magnetically pinched diodes plasma near electrodes can significantly affect electron beam focusing and Bremsstrahlung formation. (2) It is necessary to know the influence of angle spread and initial rotation of electron beam on focusing properties. (3) If gas-filled focusing cell is used, the result depends on choice of gas density. To answer the above questions PICNIC hybrid code was developed, which consists of several interrelated parts: 2D PIC code calculating dynamics of relativistic particles (electrons and ions), 3D FDTD solver for Maxwell equations, 2D MHD description for thermal electrons and ions, Monte-Carlo code PPJZMA defining particles momentum and angle after collisions. For the calculation of magnetic field the current through the anode surface is accounted. Generator parameters were the next. Diode with gas-filled focusing cell is analyzed for generator with parameters: 5 MV voltage with 30 kA current. For self-magnetically pinched diode the generator used 10.0 MV, 200 kA, 50 nsec FWHM electric pulse.Calculation results show, that diodes operate in different regimes depending on current value: initially quasi-uniform beam motion in vacuum, then unstable motion of high-current electron beam in plasma. Return current and magnitudes of local current densities inside plasma play an important role in these collective effects of beam-plasma interactions. These processes significantly depend on beam initial parameters, spread of angle velocities and energies. For rod-pinch diode incidence angles of electrons during Bremsstrahlung generation may vary in 50deg.
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