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《物理学报》2017,(4)
建立了多注电子束在空心圆柱波导中传输的理论模型,定量分析了多注电子束自电磁场力与镜像电磁场力对其角向运动的影响,并推导了考虑镜像束流影响下多注电子束的布里渊磁场.开展了模拟仿真研究,模拟与理论计算结果基本一致.研究发现:当电子束注数较少且靠近波导管壁传输时,镜像电磁场力是影响多注电子束角向漂移的主要因素;随着电子束注数或电子束与波导壁间距的增加,镜像电磁场力迅速减小并趋近于零,此时自电磁场力起主导作用;在一般情况下,漂移角速度的变化百分比只与加速电压有关,与多注电子束的注数、空间位置关系等参数无关.在输出电压约670 kV,电流约7 kA,空心圆柱波导长约100 mm的平台上开展了实验研究,研究发现多注电子束存在明显的畸变,通过进一步的分析认为多注阴极柱的侧面发射是导致电子束畸变的一个主要因素,并且二极管加速区的角向漂移不可忽视.提出并模拟验证了采取倾斜多注阴极柱的方法可提高电子束的引入效率. 相似文献
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通过箔 聚焦的电子束的包络方程研究了电子束的平衡与稳定特性,从而得到了能够传输的电子束的参数与箔之间距离和波导半径之间的关系。 相似文献
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我们研制了CEBQ程序和ENVLOP程序,模拟稳态相对论电子束在二极管区的产生和加速,以及电子束在阳极通道内的传输过程。CEBQ程序模拟二极管区电子轨道,当阳极电压为1.5MV时,阴极总发射电流为17.9kA,进入阳极通道内的传输电流为4.3kA,阳极入口处D=4cm的束发射度为24.9cm.mrad。ENVLOP程序使用线性近似下的包络方程,描述电子束包络在螺旋管引导磁场作用下的变化,讨论了外加引导磁场对包络的影响。计算结果表明,在合适引导磁场作用下,束包络起伏较小,进入阳极通道的束流(4.3kA)能全部通过。 相似文献
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本文使用一般包络方程理论推导出轴对称电子束在傍轴近似下的稳态传输过程中的发射度变化公式。结果表明电子束发射度变化与引导磁场及离子通道电场无直接关系,而仅仅与电子束分布的变化有关;发射度变化的本质是电子束的静电势能和横向运动的动能之间的转换。本文的解析结果与数值模拟结果符合得相当好。本文还定性讨论了电子束平均正则角动量对发射度变化的影响。 相似文献
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HIRFL CSR的电子冷却系统是采用强流电子束对重离子束进行冷却。在冷却段漂移管区,由于强流电子束自身的空间电荷场和螺线管磁场的作用,使得电子束的包络发生振荡。通过求解电子束的横向包络方程,研究了强流电子束包络随电子束参数和螺线管聚焦磁场的变化关系。计算结果表明:对于不同的电子束能量和磁场,电子束包络的振荡频率也不相同;在相同的条件下,磁场越强,电子束包络振荡幅度越小,电子束能量越大,其包络的振荡频率也越快。 相似文献
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以直线感应加速器(LIA)匹配磁场设计和束线调谐为背景,提出解决强流相对论电子束长距离、小波动、多元件磁约束的输运优化问题的数值优化办法,建立基于遗传算法的优化程序。结合束质心轨迹及束包络耦合模型,设计描述束传输半径波动大小的评价函数,采用励磁元件馈入电流为优化对象,解决LIA磁场配置组合爆炸优化问题。计算结果表明:优化程序可依据不同的初始束流,有针对性地快速给出一组符合束输运要求的励磁电流配置。研究成果为在建的LIA装置束线调谐提供一种重要的数值分析工具。 相似文献
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以直线感应加速器(LIA)匹配磁场设计和束线调谐为背景,提出解决强流相对论电子束长距离、小波动、多元件磁约束的输运优化问题的数值优化办法,建立基于遗传算法的优化程序。结合束质心轨迹及束包络耦合模型,设计描述束传输半径波动大小的评价函数,采用励磁元件馈入电流为优化对象,解决LIA磁场配置组合爆炸优化问题。计算结果表明:优化程序可依据不同的初始束流,有针对性地快速给出一组符合束输运要求的励磁电流配置。研究成果为在建的LIA装置束线调谐提供一种重要的数值分析工具。 相似文献
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N. D. Naumov 《Technical Physics》2000,45(9):1196-1200
A self-similar solution to the self-consistent gasdynamics equations is used to derive envelope equations for a thin curvilinear charged beam propagating in an external electromagnetic field. 相似文献
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A. S. Manuilov 《Technical Physics》2017,62(2):189-195
Kinetic methods are used to derive the transport equations, virial equation, dynamic equilibrium condition, and the equation of the envelope of an axially symmetric paraxial relativistic electron beam propagating in an Ohmic plasma channel during the evolution of resistive firehose instability. The equation of the beam envelope is generalized by taking this instability into account. 相似文献
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将电子注视为等离子体柱,从填充等离子体柱的谐振腔的物理模型出发,推导了圆柱腔填充中心电子注时TM0m0模式的特征方程,并重点分析了填充电子注的圆柱腔中TM010模式和TM020模式的谐振频率和电磁场分布随等离子频率的变化情况。研究结果表明,随着电子注的等离子体频率不断增大,谐振频率也不断增大,谐振腔内电场和磁场的分布也随之发生改变。当电子注的等离子体频率超过谐振腔的谐振频率时,谐振腔内的电磁场分布将发生很大的变化,出现了电子注内外电场方向相反和趋肤效应等现象。 相似文献
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N. D. Naumov 《Technical Physics》1998,43(1):93-96
A self-similarity approach is used to obtain envelope equations for an annular beam propagating along a magnetic field, and
also an electron beam injected at an angle to a magnetic field. An exact solution is constructed for the self-consistent problem
of transverse oscillations of a cold annular beam in a magnetic field, and a comparison is made with approximate results from
the method of envelope equations.
Zh. Tekh. Fiz. 68, 103–107 (January 1998) 相似文献
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In this paper, the coupling instability of warm relativistic electron beam (WREB) propagating through the ion channel guiding is investigated in detail. Obtaining the equilibrium state of the system by considering the self-electric and azimuthal magnetic field, the fluid-Maxwell equations as well as linear perturbation theory are employed to derive the dispersion relation of the excited modes in the system. Numerical analysis of the obtained dispersion relation shows that the electromagnetic (EM) instability can be induced nearly the center of the beam through coupling between the fast electron plasma wave (FEPW), originated from the longitudinal oscillation of WREB, and fast forward electromagnetic wave (FFEW). In this sense, growing the perturbation amplitude occurs due to transport the kinetic energy of WREB to the EM wave at the specific frequency range, where the phase velocity of FEPW and FFEW is coincided. The results of the present investigation will greatly contribute to the understanding of the stability of the warm relativistic electron beam in laboratory experiments, such as in free electron laser experiments, where the ion-channel guiding is used to confine the electrons against the self-repulsive forces generated by the beam itself. 相似文献
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Evaluation of the energy deposition region of a laser-produced relativistic electron beam in dense core plasma is essential in the fast ignition approach to ICF. Recently, we have developed a two-dimensional relativistic Fokker-Planck code “RFP-2D” for fast electron transport in dense plasmas to investigate the energy deposition profiles. In this paper, we compare the sizes of the energy deposition region derived from RFP-2D and another RFP-type calculation model with stochastic treatments. It is found to be considerably important to take into account the influence of the self-generated electromagnetic field when evaluating the energy deposition region. 相似文献
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A. S. Manuilov 《Technical Physics》2005,50(4):491-497
A kinetic approach is applied to derive the transport equations, the virial equation, the dynamic-equilibrium equation, and
the envelope equation for an axially symmetric paraxial relativistic electron beam propagating through a scattering gas-plasma
medium in the presence of a reverse plasma current with a radial density profile that is generally different from the beam
density profile. The equations obtained include additional terms that account for this difference. 相似文献