双维位置灵敏CsI(Tl)闪烁探测器

介绍了一种双维位置灵敏CsI(Tl)闪烁探测器, 利用GEANT4对它进行了蒙特卡罗模拟, 得到了RIB 17N的位置分布谱及探测器的空间位置分辨,　模拟结果与实验测量值很好地吻合。给出了影响探测器分辨的主要因素及改进方案。A two dimensional position sensitive CsI(Tl) scintillation detector readout with PSPMT was introduced. The performance of detector was simulated by using Monte Carlo code GEANT4. The position spectrum of RIB 17N and the detector’s position resolution were obtained, and the simulation results accorded with the experimental ones. The main factors, which can affect performance of the detector, and some planned detector improvements were presented.     

Position sensor based on slit imaging

A position sensor based on slit imaging is proposed and its measurement principle is described. An imaging slit is illuminated by a collimated laser beam with square-wave modulation and imaged on a detection double slit through a 4f system. A magnified image of the detection double slit is formed on a bi-cell detector. The position of the imaging slit is obtained by detecting light intensity on two parts of the hi-cell detector. In experiments, the feasibility of the sensor was verified. The repeatability was less than 40 nm.     

Design and test of SX-FEL cavity BPM

This paper reports the design and cold test of the cavity beam position monitor （CBPM） for SX-FEL to fulfill tile requirement of beam position measurement resolution of less than 1 p_m, even 0.1 btm. The CBPM was optimized by using a coupling slot to damp the TM010 mode in the output signal. Tile isolation of TM01o mode is about 117 dB, and the shunt impedance is about 200 ~@4.65 GHz with the quality factor 80 from MAFIA simulation and test result. A special antenna was designed to load power for reducing excitation of other modes in the cavity. The resulting output power of TM110 mode was about 90 mV/mm when the source was 6 dBm, and the accomplishable minimum voltage was about 200 btV. The resolution of the CBPM was about 0.1 btm from the linear fitting result based on the cold test.     

Commissioning of electron cooling in CSRe

The 400 MeV/u 12C6＋ ion beam was successfully cooled by the intensive electron beam near 1 A in CSRe.The momentum cooling time was estimated near 15 s.The cooling force was measured in the cases of difierent electron beam profiles,and the difierent angles between the ion beam and electron beam.The lifetime of the ion beam in CSRe was over 80 h.The dispersion in the cooling section was confirmed as positive close to zero.The beam sizes before cooling and after cooling were measured by the moving screen.The beam diameter after cooling was about 1 mm.The bunch length was measured with the help of the signals from the beam position monitor.The difiusion was studied in the absence of the electron beam.     

平行玻璃板对105 keV Ar7+离子的导向效应

研究了平行玻璃板对高流强（约80 nA）105 keV Ar7+离子的导向效应, 利用一维位置灵敏探测器测量了不同倾斜角下出射离子的强度及角分布。 实验结果表明, 平行玻璃板对Ar7+离子有导向作用。 与离子在微孔膜中的导向效应不同, 从平行玻璃板出射的Ar离子角分布的FWHM随着倾斜角的改变而改变, 并且出射离子角分布最大值处对应的观察角不等于倾斜角。 The transmission of 105 keV Ar7+ ions with high incident current (about 80 nA) through the gap formed by a paired parallel glass plates was investigated. The intensity and angular distribution of the transmitted ions for various tilt angles were measured using a one dimensional position sensitive detector. The results indicate the existence of a guiding effect when Ar7+ ions pass through the gap, but it is different from that for ions passing through nonacapillaries. We found a measurable dependence of the full width at half maximum (FWHM) of the transmitted ions as a function of the tilt angle. In addition, when the gap was tilted with respect to the direction of the incident beam, the observation angle related to the center of the transmitted ions profile was not equal to the tilt angle.     

THGEM探测器X光斑寻迹和位置分辨实验研究

介绍了一种基于THGEM的X射线光斑寻迹探测器,用于X射线单光子计量技术研究和测量,探测器有效面积200 mm×200 mm,采用128路基于ASIC和FPGA的高速读出电子学,探测器分为中间高分辨区和外围低分辨区两部分,两部分共用一套读出电子学。实验在中国计量科学研究院利用X光机产生的束线,测试光斑位置、光斑精细分布以及探测器的位置分辨。实验结果表明,探测器实现了同时对光斑寻迹和光斑的精细测量,探测器中间高分辨区x方向的位置分辨率为0.63 mm（FWHM）,y方向位置分辨率为0.62mm（FWHM）,探测器各项性能指标均达到了预期目标。This paper introduces the detector of X-ray spot tracing based on the THGEM. It is used for X ray single photon measurement technology research and measurement with an effective area of 200 mm×200 mm. The circuit board has 128 array of high speed readout electronics based on ASIC and FPGA. And it is divided into two parts:the middle area of high sensitive and the peripheral area of low sensitive. The two parts share a set of readout electronics. The experiment tests the position and the fine structure of the beam line produced by X ray machine in National Institute of Metrology. The results of the experimental show that the detector realizes both the spot tracing and the fine structure of the spot. The position resolution is 0.63 mm in x direction and 0.62 mm in y direction in high sensitive of the detector, which achieve the desired goal of preliminary design.     

Experiment studies on the polarized gamma-rays generation at KEK-ATF

Polarized positrons can be created through electron-positron pair creation from circularly polarized gamma-rays. Laser-Compton scattering is an effcient method to generate circularly polarized gamma-rays. A high finesse 2-mirror optical stacking cavity had been installed on the straight section of the electron storage ring at KEK-ATF. A 1064 nm circularly polarized pulsed laser beam was stacked in the cavity. Polarized gamma-rays with a maximum energy of 28.3 MeV were produced via inverse Compton scattering of the enhanced laser pulse off an electron beam of 1.28 GeV. The number of generated gamma photons per collision was estimated by a photon detector. It was found that the experimental result was in agreement with the simulated value.     

MICROMEGAS探测器初步测试

介绍了一种利用鱼线做放大区间隔的MICROMEGAS探测器, 灵敏面积为50 mm ×50 mm。 在Ar+CO₂（10%）气体条件下, 利用55Fe源5.9 keV的 X射线对MICROMEGAS探测器进行了初步测试: 计数率大于103 Hz的条件下, 计数率坪长达到280 V; 当栅极电压在800 V时能量分辨为30%; 当增益高于104时打火率低于10-4; PCB板读出条周期为400 μm条件下的位置分辨好于120 μm。 结果表明, 研制的MICROMEGAS探测器达到了初步设计的基本要求。 In this paper,A MICROMEGAS(Micro Mesh Gaseous Structure) detector with the amplification gap defined by stretching nylon fishing lines has been described . And its count plateau, gas gain and energy resolution in the condition of a 55Fe X ray source and Ar CO₂ (10%) mixture gases are measured as functions of mesh voltage. The count plateau approaches 280 V at the count rate of 103 Hz. The discharge rate is less than 10－4 when the gas gain is up to 104. The energy resolution is 30% (FWHM) based on －800 V mesh voltage. The position resolution is less than 120 μm at the condition of the sensitive area (50 mm×50 mm) Printed Circuit Boards (PCB) and its strip pitch of 400 μm. The results can satisfy the basic demand of MICROMEGAS detector preliminary design.     

Prototype of a large neutron detector based on MWPC

A prototype of large-area position sensitive neutron detector was designed and constructed according to the requirements of the Small-Angle Scattering spectrometer of China Spallation Neutron Source(CSNS).The detector was based on the 3He neutron convertor and MWPC with an effective area of 650 mm×650 mm.A prototype was completed and tested with 55Fe X-ray.The high-pressure vessel was designed and constructed with high-strength aluminum alloy.A position resolution of about 4.6mm×2.3 mm(FWHM)and efficiency65%for neutrons with wavelength of 1.8?was determined after the operational gas filled.     

Beam test of a one-dimensional position sensitive chamber on synchrotron radiation

A one-dimensional single-wire chamber was developed to provide high position resolution for powder diffraction experiments with synchrotron radiation. A diffraction test using the sample of SiO₂ has been accomplished at 1W2B laboratory of Beijing Synchrotron Radiation Source. The data of the beam test were analyzed and some diffraction angles were obtained. The experimental results were in good agreement with standard data from ICDD powder diffraction file. The precision of diffraction angles was 1% to 4.7%. Most of the relative errors between measured values of diffraction angles and existing data were less than 1%. As for the detector, the best position resolution in the test was 138 μm (σ value) with an X-ray tube. Finally, discussions of the results were given. The major factor that affected the precision of measurement was deviation from the flat structure of the detector. The effect was analyzed and the conclusion was reached that it would be the optimal measurement scheme when the distance between the powder sample and detector was from 400 mm to 600 mm.     

宏观尺寸弯曲石英管对中低能电子束的导向作用

研究了宏观尺寸的弯曲圆柱形石英管对 1 100, 1 300和1 500 eV 3种能量电子束的导向作用, 并对实验结果与相同材质和尺寸的直管的情形进行了分析对比。 实验中利用一个位置灵敏法拉第筒对从石英管出射的电子束进行探测, 获得从管道中出射的电子束流强度在位置灵敏法拉第筒各道上的分布, 其结果显示宏观尺寸石英管对电子束存在导向作用。 与慢速高电荷态离子和绝缘毛细管相互作用的物理过程类似, 这种导向效应是由电荷在管壁内表面自组织充电引起的。 实验还发现, 入射电子束流的强度越强, 其导向作用越明显, 这与微观尺寸毛细管对慢速高电荷态离子的导向作用不同。 石英管导向能力与管的尺寸、 形状及材料之间的关系还有待进一步的系统研究。 It was inevstigated in the experiment that the guiding effect of electron beam with energy of 1 100, 1 300 and 1 500 eV through a bended cylindrical quartz tube with macro sized. A position sensitive Faraday cup was developed and used to detect the electron beam transmitted through the quartz tube, and the distribution of transmitted beam current on each channel of the Faraday cup was acquired. Results indicate the existence of guiding effect which is due to the self organized charge up in the inner wall of the quartz tube similar to that of the highly charged ions. We also found that the guiding ability of the tube is related to the incident beam intensity. The relationship between the guiding ability and the material as well as the size of the tube is to be studied in the near future.     

Position sensor based on slit imaging

A position sensor based on slit imaging is proposed and its measurement principle is described.An imaging slit is illuminated by a collimated laser beam with square-wave modulation and imaged on a detection double slit through a 4f system.A magnified image of the detection double slit is formed on a bi-cell detector.The position of the imaging slit is obtained by detecting light intensity on two parts of the bi-cell detector.In experiments,the feasibility of the sensor was verified.The repeatability was less than 40 nm.     

Photoluminescence properties of size-selected Si nanocluster films prepared by laser ablation

Size-dispersed Si nanocluster films have been synthesized by a method of crossing an Ar gas beam perpendicularly to a silicon cluster beam that is produced by a laser ablation technique. Flight directions of the nanoclusters are changed due to Ar gas collisions, and smaller nanoclusters are deflected further from the axis of the primary cluster beam. The size-dispersed nanocluster films exhibit strong red photoluminescence (PL) after exposure to the air. The PL peak energy changes between 1.42 and 1.72 eV depending on the sample position. The average diameter of the oxidized nanoclusters characterized by transmission electron microscopy is 10 nm at the position of the primary cluster beam axis and becomes smaller as deviated from the axis. The relation between the PL peak energy and the size of the oxidized Si nanoclusters is discussed. Received: 4 May 2000 / Accepted: 9 May 2000 / Published online: 13 July 2000     

Dynamics of VUV spectra in fast capillary discharge

The temporal behavior of VUV spectra of capillary discharge with a rate of a current rise on the order of 10¹² A/s is studied. The current is generated using an inductive storage unit with a plasma-erosion opening switch. This discharge is accompanied by the generation of a shock wave on an inner wall of a capillary and by its subsequent cumulation on the discharge axis. The capillary is prefilled with argon at a pressure of 80 Pa. Radiation spectra are obtained using an off-Rowland spectrograph based on a concave grating with optimal focusing in the wavelength range of 20 nm. The radiation is recorded with a detector based on a microchannel plate with a time resolution of 20 ns, which makes it possible to separate the spectra of two phases of the discharge, i.e., the cumulation phase of the shock wave in argon that fills the capillary (T _e ∼ 20–30 eV) and the phase of subsequent discharge in a substance desorbed from the capillary wall T _e ∼ 50 eV).     

强流重离子束在轴对称电场中的温度和能量展宽

本文研究带电粒子束在轴对称电场(包含束空间电荷平均场)中的温度和能量展宽,所得结果表明,在漂移区内,此种能量展宽与束电流成正比,与束的宏观流动速度成反比,因此,对于强流重离子束而言,此种能量展宽在总的能量展宽中将起重要的作用,若束能为20keV,束流为20mA,在漂移区中,¹H离子束的能量展宽为26.5eV,而相同条件下的¹²¹Sb离子束则为291.5eV,而且随束流增加线性上升,本文对束温度的研究结果表明,在漂移区中,束空间电荷效应使束温度增加。 关键词：     

PPAC在单粒子效应地面模拟实验中对束流均匀度测量的应用

单粒子效应(SEE)加速器地面模拟需要离子束具有较好的均匀度,针对回旋加速器单粒子效应模拟的束流特点,建立了一套以位置灵敏平行板雪崩探测器(Parallel Plate Avalanche Counter,PPAC)为基础的均匀度探测系统并完成了带束测试,对它的结构、工作原理、均匀度获得方法及带束测试结果进行描述。为验证PPAC测量结果准确性,在带束测试过程中,前方同时放置PET膜测量穿过PPAC探测器的粒子分布,与离子径迹测量结果对比,给出PPAC的均匀度的测量误差在5%之内。探测器具有50 mm×50 mm的灵敏面积和小于1 mm的位置分辨,符合单粒子效应实验对束流均匀度测量的要求。     

Surface extended electron loss fine structure: dependence on incident electron energy and collection solid angle

Reflected electron energy loss fine structure above the M_2,3 core excitation edge of Cu is measured using two dissimilar electron detection systems, a cylindrical mirror analyzer and an hemispherical grid detector, at primary energies ranging from 700 to 2000 eV. We find slight differences in the loss structures measured by the two detector systems, but the radial and pseudo-radial distribution functions calculated by an EXAFS type analysis of the extended fine structure show agreement in the first peak position to within ±0.02 Å for all primary energies above 800 eV. Core-loss and fine-structure signals from sub-monolayers of C and O were observed. No fine structure was measurable for core-loss signals of single monolayer coverages of Na, K, Cs, or S.     

金属杂质辅助低能氩离子束诱导蓝宝石自组织纳米结构

使用实验室自主研发的等离子抛光与刻蚀系统,研究了不同入射能量下不锈钢杂质辅助Ar+离子束刻蚀蓝宝石表面自组织纳米结构的形成机制.采用Taylor Surf CCI2000非接触式表面测量仪和原子力显微镜分别对刻蚀后蓝宝石样品的粗糙度、纳米结构的纵向高度和表面形貌进行了分析.研究表明:引入不锈钢杂质后,当离子束入射角度为...     

Pixelated transmission‐mode diamond X‐ray detector

Fabrication and testing of a prototype transmission‐mode pixelated diamond X‐ray detector (pitch size 60–100 µm), designed to simultaneously measure the flux, position and morphology of an X‐ray beam in real time, are described. The pixel density is achieved by lithographically patterning vertical stripes on the front and horizontal stripes on the back of an electronic‐grade chemical vapor deposition single‐crystal diamond. The bias is rotated through the back horizontal stripes and the current is read out on the front vertical stripes at a rate of ～1 kHz, which leads to an image sampling rate of ～30 Hz. This novel signal readout scheme was tested at beamline X28C at the National Synchrotron Light Source (white beam, 5–15 keV) and at beamline G3 at the Cornell High Energy Synchrotron Source (monochromatic beam, 11.3 keV) with incident beam flux ranges from 1.8 × 10^?2 to 90 W mm^?2. Test results show that the novel detector provides precise beam position (positional noise within 1%) and morphology information (error within 2%), with an additional software‐controlled single channel mode providing accurate flux measurement (fluctuation within 1%).     

低能电子在外层导电屏蔽的玻璃锥管中的传输

采用新的具有常数锥角的玻璃锥管,并对玻璃锥管进行了外表面导电屏蔽,通过对电子穿越玻璃锥管的二维角分布随时间演化的观测,研究了低能电子与玻璃管相互作用的机制.发现电子穿越完全放电的玻璃锥管时穿透率先下降后平稳,整个过程中角分布中心发生微小移动,但角分布的半高宽几乎保持不变.这与我们之前发表的工作(2016 Acta Phys.Sin.65 204103)不同,这是由于对玻璃锥管进行外表面导电屏蔽会阻止外界不确定的快速充放电的影响,并形成了新的稳定放电通道,有利于实现电子的稳定穿透.电子的穿透率随倾角呈类似矩形的分布,透射电子的角分布中心伴随倾角的变化而移动,其穿透所容许的倾角与几何穿透一致.