Afsharmanesh M, Habibi M
Department of Energy Engineering and Physics, Amirkabir University of Technology, Tehran, Iran.
Rev Sci Instrum. 2018 Mar;89(3):033301. doi: 10.1063/1.5010010.
In the present context, the extraction system of a helicon ion source has been simulated and constructed. Results of the ion source commissioning at up to 20 kV are presented as well as simulations of an ion beam extraction system. Argon current of more than 200 μA at up to 20 kV is extracted and is characterized with a Faraday cup and beam profile monitoring grid. By changing different ion source parameters such as RF power, extraction voltage, and working pressure, an ion beam with current distribution exhibiting a central core has been detected. Jump transition of ion beam current emerges at the RF power near to 700 W, which reveals that the helicon mode excitation has reached this power. Furthermore, measuring the emission line intensity of Ar ii at 434.8 nm is the other way we have used for demonstrating the mode transition from inductively coupled plasma to helicon. Due to asymmetrical longitudinal power absorption of a half-helix helicon antenna, it is used for the ion source development. The modeling of the plasma part of the ion source has been carried out using a code, HELIC. Simulations are carried out by taking into account a Gaussian radial plasma density profile and for plasma densities in range of 10-10 m. Power absorption spectrum and the excited helicon mode number are obtained. Longitudinal RF power absorption for two different antenna positions is compared. Our results indicate that positioning the antenna near to the plasma electrode is desirable for the ion beam extraction. The simulation of the extraction system was performed with the ion optical code IBSimu, making it the first helicon ion source extraction designed with the code. Ion beam emittance and Twiss parameters of the ellipse emittance are calculated at different iterations and mesh sizes, and the best values of the mesh size and iteration number have been obtained for the calculations. The simulated ion beam extraction system has been evaluated using optimized parameters such as the gap distance between electrodes, electrodes aperture, and extraction voltage. The gap distance, ground electrode aperture, and extraction voltage have been changed between 3 and 9 mm, 2-6.5 mm, and 10-35 kV in the simulations, respectively.
在当前背景下,对螺旋波离子源的引出系统进行了模拟和构建。给出了高达20 kV时离子源调试的结果以及离子束引出系统的模拟结果。在高达20 kV的电压下引出了超过200 μA的氩离子流,并用法拉第杯和束流轮廓监测栅进行了表征。通过改变不同的离子源参数,如射频功率、引出电压和工作压力,检测到了具有中心芯部电流分布的离子束。离子束电流在接近700 W的射频功率处出现跳跃转变,这表明螺旋波模式激发已达到该功率。此外,测量Ar ii在434.8 nm处的发射线强度是我们用于证明从电感耦合等离子体到螺旋波模式转变的另一种方法。由于半螺旋螺旋波天线的纵向功率吸收不对称,它被用于离子源的开发。使用HELIC代码对离子源的等离子体部分进行了建模。通过考虑高斯径向等离子体密度分布以及10^10 m范围内的等离子体密度进行了模拟。获得了功率吸收谱和激发的螺旋波模式数。比较了两种不同天线位置的纵向射频功率吸收。我们的结果表明,将天线靠近等离子体电极放置有利于离子束引出。使用离子光学代码IBSimu对引出系统进行了模拟,这使其成为首个用该代码设计的螺旋波离子源引出系统。在不同的迭代次数和网格尺寸下计算了离子束发射度和椭圆发射度的Twiss参数,并获得了计算的最佳网格尺寸和迭代次数值。使用诸如电极之间的间隙距离、电极孔径和引出电压等优化参数对模拟的离子束引出系统进行了评估。在模拟中,间隙距离、接地电极孔径和引出电压分别在3至9 mm、2至6.5 mm和10至35 kV之间变化。