共查询到20条相似文献,搜索用时 93 毫秒
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在MIT型漂移室单元中, 利用Naples扁平型线绕延迟线进行了第二坐标, 即沿阳极丝方向的位置读出性能测试. 使用P9或Ar/CH4=70/30工作气体, 沿长度为80cm的延迟线测量到的空间分辨为2~5mm, 位置读出线性优于1%. 相似文献
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利用宇宙线分别研究了一个小单元漂移室在He/C3H8(60/40)和He/CH4(60/40)两种氦基混合气下的性能.作为比较还测试了在Ar/CO2/CH4(89/10/1)混合气下的性能.研究表明上述氦基混合气的空间分辨和dE/dx分辨好于Ar/CO2/CH4(89/10/1)混合气.使用He/C8H8(60/40)可以获得110μm的空间分辨,在30—40次取样下dE/dx分辨可以达到6%—7%. 相似文献
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小单元漂移室用放射源模拟老化的实验研究 总被引:2,自引:0,他引:2
BESⅢ 漂移室(DC)模型用1.85X109 Bq 55Fe 5.9keV X射线放射源作加速老化实验研究.测量了阳极丝电流I和55Fe 5.9keV X射线全能光电峰位随累积电荷量Q的变化,由此得到累积相当BESⅢ DC 5年全天候运行的电荷量(0.07 C/cm)后,漂移室小单元的阳极电流降为初始值的87%;老化率为R=-0.19%/(mC/cm) 相似文献
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微型差动式共焦自聚焦光聚焦探测系统 总被引:1,自引:0,他引:1
为解决微小内轮廓尺寸为代表的微小尺寸的非接触式超精密测量问题,提出了将自聚焦透镜体积小的特点与共焦显微技术的高分辨率和绝对位置跟踪特性相结合的差动式自聚焦共焦微型显微技术的光探测技术,建立了相应的传感系统,介绍了系统的工作原理和构成,自聚焦透镜测头直径为1mm,两个探测器差动设置,不但消除了光源的光强漂移和探测器的电子漂移产生的共模噪声,提高了测量信噪比,而且有效地提高了系统的轴向分辨率,初步实验表明,系统轴向分辨率在倾斜率小于20度的范围内可达5nm。 相似文献
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A stopping layer concept to improve the spatial resolution of gas-electron-multiplier neutron detector 下载免费PDF全文
Jianjin Zhou 《中国物理 B》2022,31(5):50702-050702
In recent years, gas electron multiplier (GEM) neutron detectors have been developing towards high spatial resolution and high dynamic counting range. We propose a novel concept of an Al stopping layer to enable the detector to achieve sub-millimeter (sub-mm) spatial resolution. The neutron conversion layer is coated with the Al stopping layer to limit the emission angle of ions into the drift region. The short track projection of ions is obtained on the signal readout board, and the detector would get good spatial resolution. The spatial resolutions of the GEM neutron detector with the Al stopping layer are simulated and optimized based on Geant4GarfieldInterface. The spatial resolution of the detector is 0.76 mm and the thermal neutron detection efficiency is about 0.01% when the Al stopping layer is 3.0 μ m thick, the drift region is 2 mm thick, the strip pitch is 600 μ m, and the digital readout is employed. Thus, the GEM neutron detector with a simple detector structure and a fast readout mode is developed to obtain a high spatial resolution and high dynamic counting range. It could be used for the direct measurement of a high-flux neutron beam, such as Bragg transmission imaging, very small-angle scattering neutron detection and neutron beam diagnostic. 相似文献
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为获取超快光脉冲信号,提出了一种基于光电子脉冲准线性展宽的高时间分辨二维成像技术。利用高频时变电场的线性工作区加速光电子脉冲信号,通过优化阴极激励源的电参数,选择光电子进入加速区的时刻实现光电子脉冲的准线性展宽。利用曝光时间100ps的门控选通微通道板在脉冲展宽模块的记录面进行选通曝光成像,实现高时间分辨的二维成像。为改善系统的空间分辨和成像畸变,添加轴向聚焦磁场解决电子漂移区中由电子空间电荷效应引起的时间和空间弥散,对于能量4 keV、出射角0.1°的电子束,聚焦磁场的最佳强度为0.057 T,此时阴极中心位置的空间分辨可达5 1p/mm,阴极边缘位置空间分辨稍差。基于光电子脉冲准线性展宽技术,可将漂移距离50 cm,初始脉宽10 ps的电子脉冲展宽10倍,从而可将门控MCP探测器的时间分辨提高1个量级(即10 ps以内)。 相似文献
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Tests on the read out of the second coordinate (along the anode wire) of the MIT-Harward-type drift chamber by using a Naples type flat solenoieal delay line were conducted. Spatial resolution of 2~5mm and linearity better than 1% were obtained along the delay line of 80cm in length with the gas mixture of P9 or Ar/CH4=70/30. 相似文献
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The two dimensional drift chamber was formed by gluing a delay-line in a MIT-Harvard type drift chamber. An average drift velocity about 3.34cm/μs was obtained when the chamber was operated at plateau region and filled with P-9 gas. Its average space resolution is 570μm. The output signal amplitude of the chamber being changed when alter the incident particle's (both β- and X-ray) position was observed. 相似文献
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在气体探测器研究中,利用266 nm紫外激光的双光子电离物理机制使气体电离产生可测量的信号,是一种重要的标定方法.随着微结构气体探测器(MPGD)的不断发展,用紫外激光标定来实现较高精度位置分辨率成为了一种研究需求,对此有两个关键技术问题需要解决:实验研究激光可测信号大小以及激光指向精度.分析和模拟计算了紫外光电离信号大小和激光调光误差,基于微结构气体电子倍增器探测器与266 nm波长激光束,在工作气体Ar/CO_2(70/30)中,测量了不同光斑面积与输出信号的关系;设计和研制了紫外激光调光系统,实验测量了紫外光调光偏差.模拟结果与实验结果对比分析表明:紫外激光束作用于气体探测器,探测器增益在5000,前放增益为10 mV/fC时, 6 mm读出条宽输出信号幅度约400 mV;在探测器内传播距离为400 mm时,较短时间内(10—20 min)实验调光指向精度可以保证小于5′,引入z向偏差最大可以达到0.33 mm,对应z向漂移速度的测量相对误差为6.4×10-4.该研究为MPGD与紫外激光标定实验设计提供主要的设计参考. 相似文献
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Using a DC-biased room-temperature photoconductive switching element, a picosecond resolution optical streak camera is operated at sweep rates up to 7 ps/mm. Single-shot jitter is 2 ps with complete absence of short and long-term drift characteristic of all other sweep drivers. This high accuracy allows the streak camera to be used in a single-shot averaging mode which leads to a sub-picosecond absolute timing accuracy. When operated in this manner, the streak camera becomes a highly reliable and accurate device for measuring transient events on a time scale of single picoseconds. The simplicity of this method makes it highly attractive for many applications in laser fusion and picosecond chemistry and photophysics studies where reliable no-drift operation is highly desirable. 相似文献
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