Abstract

<sec>It is a hot topic that using glass capillary to focus and shape the charged particle beam, for it is inexpensive and simple. There are the cases that single glass capillaries are used to make the microbeam of the positive ions. When it comes to electrons, their transmitting through insulating capillaries is complex and the attempt to use the glass capillary to produce electron beams in the size of micrometer needs further exploring.</sec><sec>In this paper, the charging-up process of the 900-eV electrons transmitting through a glass capillary with the grounded conductive-coated outer surface is reported. Two-dimensional angular distributions of the transmitted electrons and their time evolutions are measured for the cases of various tilt angles of glass tube. It is found that there are a considerable number of transmitted electrons at the tilt angle exceeding the geometrical opening angle (1°) of the glass tube. The intensity of transmitted electrons for large tilt angle (i.e. –1.15°) can be considered as first falling to zero, then keeping zero for a long time, finally rising to a certain stable value. Correspondingly, the angular distribution center experiences moving towards negative-positive-negative-settled. The energy losses are measured for various tilt angles. The larger the tilt angles, the larger the energy loss of transmitted electrons is. To better understand the physics behind the observed phenomena, the simulations of the energy loss for transmitted electrons at various tilt angles are performed by the Monte Carlo method. The comparation between the simulated energy losses and the measured energy losses shows that the experimental results are well explained by multiple deflections from the wall.</sec>

Highlights

  • The X-axis stands for the absolute value of the voltage of the analysis mesh

  • The circles represent the experimental data, and the black lines stand for the calculation data after various times reflection

  • 由于在测量过程中没有经过放电,正角度方向管壁体内沉积的负电荷是持续 累积的,即第一次反射所需的负电荷量在-0.15度倾角的充电过程中已基本累积完 成并在后续倾角下还会再次累积。因此随着倾角远离0度,第一次反射所需的充 电时间会越来越短,也即测量中显示的倾角越远离0度,穿透率下降至最低点所 经历的充电时间越短。而倾角远离0度后,由于反射角的增大,负角度方向的管 壁总会有一部分从未累计过电荷,即每个倾角下,第二次反射所需的电量基本都 需要从0累积。在负电荷累积到可以排斥后续入射电子穿出管壁表面前,穿透率 都会在最低点保持不变。倾角越远离0度,反射需要的负电场越强,所以第二次 反射需要的充电时间也越多。因此在-0.4度和-1.15度倾角下,会测量到穿透率接 近于零的时段,并且倾角越大,持续时间越长。

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Introduction

李鹏飞 1) 袁华 1) 程紫东 1) 钱立冰 2) 刘中林 1) 靳博 1) 哈帅 1) 张浩 文 1) 万城亮 1) 崔莹 1) 马越 3) 杨治虎 4) 路迪 5) Reinhold Schuch 6) 黎 1)(兰州大学核科学与技术学院,兰州 730000) 2)(湖北科技学院核技术与化学生物学院,咸宁 437100) 3)(RIKEN Nishina Center, RIKEN, Wako, 351-0198, Japan) 4)(中国科学院近代物理研究所,兰州 730000) 5)(Department of Physics, University of Gothenburg, SE-41296 Gothenburg, Sweden) 6)(Physics Department, Stockholm University, SE-10691 Stockholm, Sweden)

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