基于各向异性和后加速技术的100fs时间分辨条纹管设计

None Tian Li-Ping, None 陈萍, None Shen Ling-bin, None Chen Ping, None Liu Yu-zhu, None Chen Lin, None Hui Dan-dan, None Chen Xi-ru, None Zhao Wei, None Xue Yan-hua
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引用次数: 0

摘要

减小扫描偏转系统边缘场效应引起的空间电荷效应和时间色散是实现100飞秒条纹管的关键。本文提出并设计了一种新型飞秒条纹管。对影响时间分辨率的因素进行了理论分析,并给出了技术指标。对两种常见加速系统结构(平面阴极-网状加速电极和平面阴极-狭缝加速电极)上的电场分布和电子透射率等参数进行了理论比较和分析。结果表明:平面阴极网状加速电极形成的电场分布虽然能形成均匀的电场,但电子透过率很低;平面阴极-狭缝加速结构会使光电子束沿扫描方向离焦,但阴极有效探测范围内的电子透过率高达100%。光电子束的散焦可以通过在阳极前面设置一个窄缝来消除。聚焦电极采用前后垂直放置的两组板状结构,分别沿扫描方向和狭缝方向形成一维聚焦电场。空间聚焦电极靠近荧光粉屏放置,有利于将电子束的交叉点沿空间方向推回。因此,在电子密度较大的情况下,电子的传递时间色散会减小。同时,阳极可提供+5000 V的后加速电压,有利于缩短光电子的传输时间和色散,从而提高时间分辨率。在上述理论分析的基础上,采用平面阴极-狭缝加速电极、各向异性聚焦系统和后加速方法设计了一种新型飞秒条纹管。模拟了阳极狭缝宽度对空间分辨率和时间分辨率的影响。结果表明,时间分辨率随着阳极狭缝宽度(10 μm ~ 50 μm)的增大而下降,这是由于阳极狭缝宽度的增大会导致电子光斑沿扫描方向的尺寸逐渐增大,从而导致技术时间色散增大。此外,本文还给出了阳极狭缝宽度在10~50 μm范围内飞秒条纹管的仿真结果。结果表明:静态空间分辨率高于100 lp/mm @ MTF=10%,动态空间分辨率高于29 lp/mm @ MTF=10%,在4 mm阴极有效探测长度范围内,时间分辨率优于122 fs。当阴极有效探测长度增加到8 mm时,条纹管的动态空间分辨率高于22 lp/mm @ MTF=10%,时间分辨率优于191 fs。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
100 fs time-resolved streak tube design based on anisotropy and post-acceleration technology
Reducing the space charge effect and the time dispersion caused by the edge field effect of the scanning deflection system is the key to realize the 100-femtosecond streak tube. In this paper, a novel femtosecond streak tube is proposed and designed. The factors affecting the temporal resolution are analyzed theoretically and the specifications are given. Parameters including the electric field distribution and electron transmittance on the two common acceleration system structures (planar cathode -mesh accelerating electrode and planar cathode – slit accelerating electrode) are compared and analyzed theoretically. The results show that although the electric field distribution formed by the planar cathode – mesh accelerating electrode could form uniform electric field, the electron transmittance is very low; planar cathode-slit accelerating structure would defocus the photoelectron beam along the scanning direction, but the electron transmittance in the effective detection range of the cathode is as high as 100%. The defocusing of the photoelectron beam can be removed by setting a narrow slit in front of the anode. The focusing electrode adopts two groups of plate-like structures which are vertically placed front and back, forming one-dimensional focusing electric fields along the scanning and the slit direction, respectively. The spatial focusing electrode is placed close to the phosphor screen, which is beneficial to push back the cross-point of the electron beam along the spatial direction. Thus, the electron transit time dispersion in the condition of large electron density would decrease. At the same time, the anode can provide a post-accelerating voltage of +5000 V, which is beneficial to shorten the transit time and dispersion of the photoelectrons, thereby improving the temporal resolution. Based on the above theoretical analysis, a novel femtosecond streak tube is designed by using planar cathode-slit accelerating electrode, anisotropic focusing system and post-accelerating method. The influence of the anode slit width on the spatial and temporal resolution is simulated. The results show that the temporal resolution deteriorates with the increase of the anode slot width (10 μm ~ 50 μm), due to the increase of the anode slit width will lead to the gradual increase of the size of the electron spot along the scanning direction, which would lead to the increase of the technical time dispersion. In addition, this study gives the simulation results of the femtosecond streak tube when the anode slit width is in the range of 10~50 μm. The results show that the static spatial resolution is higher than 100 lp/mm @ MTF=10%, dynamic spatial resolution is higher than 29 lp/mm @ MTF = 10%, the temporal resolution is better than 122 fs in the range of 4 mm cathode effective detection length. When the effective detection length of the cathode is increased to 8 mm, the dynamic spatial resolution of the streak tube tube is higher than 22 lp/mm @ MTF=10%, and the temporal resolution is better than 191 fs.
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