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本文采用SLAC-226程序计算了1.5MV强流电子束在二极管内的加速过程以及出阳极后的传输过程。高亮度二极管的设计是高效率自由电子激光的关键技术之一。本工作的目的就是通过1.5MV注入器的数值模拟,为寻找优化的二极管结构设计提供一种有效的数值方法。程序考虑了外加电磁场和电子束自身空间电荷和自生磁场效应。我们讨论了外加磁场的各种构形以及它们对束流品质的影响,计算结果与国外EBQ程序计算结果和实验结果进行了比较,证明本工作的结果是可靠的。SLAC-226程序可以为直线感应加速器的设计提供参考数据。 相似文献
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采用粒子模拟(PIC)方法模拟了强流电子束在薄磁透镜中的聚焦。建立了强流电子束的聚焦模型,模拟了神龙一号加速器某次实验的结果,得到的模拟结果非常接近实验值,证明采用建立的PIC模型模拟强流束经过磁透镜时的聚焦是可信的。应用此模型模拟了电子束参数(入射半径、发射度、能散度、相位角等)对焦斑直径的影响, 结果表明:在模拟条件下,电子束平行入射时最佳束包络半径位于20.0~22.5 mm;发射度和能散度对焦斑直径的影响和理论公式吻合得较好;只有入射电子束包络半径和相位角匹配时才能得到小的焦斑直径。 相似文献
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采用粒子模拟(PIC)方法模拟了强流电子束在薄磁透镜中的聚焦。建立了强流电子束的聚焦模型,模拟了神龙一号加速器某次实验的结果,得到的模拟结果非常接近实验值,证明采用建立的PIC模型模拟强流束经过磁透镜时的聚焦是可信的。应用此模型模拟了电子束参数(入射半径、发射度、能散度、相位角等)对焦斑直径的影响, 结果表明:在模拟条件下,电子束平行入射时最佳束包络半径位于20.0~22.5 mm;发射度和能散度对焦斑直径的影响和理论公式吻合得较好;只有入射电子束包络半径和相位角匹配时才能得到小的焦斑直径。 相似文献
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由等离子体引出强流离子束的光学数值模拟 总被引:2,自引:2,他引:0
本文叙述了中性束注入器中的强流离子源引出系统离子束光学性质的数值模拟方法,并给出了典型计算结果。计算结果表明:用这种方法能反映强流离子源引出系统最本质的束光学性质,可供选取和研究强流离子束光学系统之用。 相似文献
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根据曙光一号自由电子激光实验的需要,将国外二维EBQ程序发展为三维强流束数值模拟程序(CEBQ)。CEBQ既能计算轴对称问题,还能计算磁四极子、束流偏轴和斜入射等三维问题。对强流束的自生电磁场效应,与EBQ程序一样,只考虑线性近似而略去了高阶项。使用CEBQ程序对曙光一号装置进行了计算,对摇摆器入口处的椭圆形挡板进行了论证。数值结果表明,椭圆形档板对提高束流品质,有效地产生自由电子激光是必要的。这一结果和第二轮曙光一号实验的测量结果基本一致。 相似文献
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建立了内靶对兰州冷却储存环主环束流影响的单粒子跟踪模拟程序,对pellet小丸靶和碳靶对束流带来的负面影响进行了模拟研究,主要讨论CSRm内靶实验中的束流存活率和束流寿命状态。结果显示利用厚度为1×1016 atoms×cm-2小丸内靶时,2.6 GeV质子束流寿命在100 s量级,而对于目前技术水平下的碳膜靶 (厚度为 5×1017 atoms×cm-2),质子束流寿命为s量级;束流寿命和束流能量基本成正比关系,束流寿命和内靶厚度近似成反比关系。 相似文献
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利用拟合实验测得的TEMP Ⅱ型加速器磁绝缘二极管电压波形及其焦点附近束流密度曲线,建立了Gauss分布模型.采用Monte Carlo方法研究了强流脉冲离子束与铝材镀有不同厚度金膜的双层靶(金膜与铝材合称为双层靶)之间的相互作用,模拟了能量沉积的演化过程和随不同金膜厚度的变化情况.对脉冲离子束强化薄膜粘结性进行了探讨.
关键词:
强流脉冲离子束
双层靶
能量沉积
Monte Carlo方法 相似文献
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�ŷ�꣬�ų��� 《核聚变与等离子体物理》2015,35(3):284-288
The ion beam focused state is studied theoretically by combining the schematic of the charge lens in space and the magnetohydrodynamics equation of the ion beam. The theory applies laminar flow of non-collision model to calculate a series of parameters, such as the initial radius, the emergence angle, the focal length and the minimum radius of the focal spot. The effects of energy divergence and dispersion differs on the minimum radius of the focal spot are analyzed theoretically. Finally, in line with the principles of the conservation of energy and angular momentum, the maximum radius of the beam in view of different incidence angles of the ion beam are calculates. The results show that with the increase of incident angle, the confluence angle and the minimum radius of the focal spot will reduce, and the focal length will increase. Besides, when beam radius increases, the parameters above will increase. The minimum focal spot radius, within the smooth area, is in close relationship to the energy divergence and the divergence. The larger energy divergence and the divergence become, the larger the focal length will be. Besides, beam divergence with the same incidence angle will show common character on the maximum radius. 相似文献
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《Current Applied Physics》2015,15(12):1599-1605
In this paper, we have investigated the feasibility of the high current beam extraction from anode spot plasma as an ion source for large area ion implantation. Experiments have been carried out with the ambient plasma produced by inductive coupling with radio-frequency (RF) power of 200 W at the frequency of 13.56 MHz. Anode spot plasmas are generated near the extraction hole of 2 mm in diameter at the center of a bias electrode whose area exposed to the ambient plasma can be changed. It is found that the maximum ion beam current is extracted at the optimum operating pressure at which the area of bias electrode exposed to ambient plasma is fully covered with the anode spot plasma whose size is dominantly determined by the operating pressure for given gas species. It is also observed that the extracted ion beam current increases nonlinearly with the bias power due to the changes in size and shape of the anode spot plasma. With the well-established anode spot plasma operating at the optimum gas pressure, we have successfully extracted high current ion beam of 6.4 mA (204 mA/cm2) at the bias power of 22 W (∼10% of RF power), which is 43 times larger than that extracted from the plasma without anode spot. Based on the experimental results, criteria for electrode design and operating pressure for ion beam extraction from larger extraction aperture are suggested. In addition, the stability of anode spot plasma in the presence of ion beam extraction through an extraction hole is discussed in terms of the particle balance model. 相似文献
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根据Sigmund溅射能量沉积理论建立了低能离子入射光学元件引起的能量扰动层厚度模型.理论推导了离子束倾斜入射时光学元件表面的束流密度,并建立了低能离子束对光学元件的热量沉积模型.采用MonteCarlo方法模拟了低能离子与熔石英光学表面的相互作用.分析了离子能量、离子类型、入射角度等参数对光学元件热量沉积和扰动层深度的影响规律.以离子束沉积在工件的能量作为热源,采用有限元分析软件ANSYS模拟了离子束入射工件的温度场分布、温度梯度场分布和温度应力分布.入射表面温度和热梯度呈高斯分布,束斑中心最高并向工件边缘逐渐减小.入射表面束斑区域受热膨胀,其膨胀受到外环区域的制约,从中心区域到大约束斑半峰值半径的区域,所受环向应力为压应力,在大致束斑半峰值半径以外区域为拉应力. 相似文献
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The focusing properties of the hyperbolic-cosine-Gaussian beam, which contains an optical vortex induced by a non-spiral phase plate, are investigated numerically. The phase plate alters phase distribution linearly in a half-section part of the hyperbolic-cosine-Gaussian beam, which results in one non-spiral optical vortex. Results show that the phase variation rate of the non-spiral phase plate influences focal intensity distribution considerably, and some novel focal patterns, such as line focal spot, “H”-shape focal spot, and intensity peaks array, may occur. Focal shift, focal split, and focal switch appear in focal evolution with increasing phase variation rate. The focal evolution differs for different parameters in cosh parts of the hyperbolic-cosine-Gaussian beam. For big parameters in cosh parts, the value of local intensity peaks is comparable to that of maximum intensity peaks. 相似文献