Advanced Search

WEI Xin, WANG Xiaodong, CHENG Kai, DIAO Weizhuo, CHEN Guoxiang, HE Sanjun, LI Tingting, ZHAO Yue, LIU Zheng. Monte Carlo Simulation on the Novel M-THGEM Detector[J]. Nuclear Physics Review, 2019, 36(1): 85-90. doi: 10.11804/NuclPhysRev.36.01.085
Citation: WEI Xin, WANG Xiaodong, CHENG Kai, DIAO Weizhuo, CHEN Guoxiang, HE Sanjun, LI Tingting, ZHAO Yue, LIU Zheng. Monte Carlo Simulation on the Novel M-THGEM Detector[J]. Nuclear Physics Review, 2019, 36(1): 85-90. doi: 10.11804/NuclPhysRev.36.01.085

Monte Carlo Simulation on the Novel M-THGEM Detector

doi: 10.11804/NuclPhysRev.36.01.085
Funds:  National Natural Science Foundation of China(11605086,11875163); Natural Science Foundation of Hunan Province, China(2018JJ3422); Research Foundation of Education Bureau of Hunan Province, China(15B205, 18C0461)
  • Received Date: 2018-10-30
  • Rev Recd Date: 2019-01-31
  • Publish Date: 2019-03-20
  • Compared to THGEM (Thick Gas Electron Multiplier), the novel Multilayer Thick Gaseous Electron Multiplier (M-THGEM) has many advantages, such as continuous avalanche zone, more compact structure, high gain at low pressure and low operating voltage, and easy to make large-area production. In the presented work, two types of the M-THGEM detector (two or three layers) were modeled, and their main principle and performances were also studied by simulation. Two types of the detector were molded and simulated by using the finite element software (ANSYS), and the electric field distribution and nodes information lists were figured out. The effective gain and induced signal from M-THGEM detector at different gas pressures and operating voltages were studied with the Garfield++ package. The simulation results shown that M-THGEM can obtain a stable higher gain around 105 in an environment where has a low pressure even in 200 Torr and within a pure inertia gas such as He. At this condition, the width of the induced signal from the three-layers structure is around 120 ns. Additionally, an asymmetric way of the applied voltage was studied and aim to reduce the efficiency of ion feedback, and our results show that this method is effective.
  • [1] SAULI F. Nucl Instr and Meth, 1997, 386(2):531.
    [2] WANG Xiaodong, YANG Herun, REN Zonggou, et al. Chinese Physics C, 2015, 39(2):39.
    [3] WANG Xiaodong, ZHANG Junwei, HU Bitao, et al. Chinese Physics Letters, 2015, 32(3):30.
    [4] COIMBRA A E C, HENRIQUES C A O, ISRAELASHVILI I, et al. Journal of Instrumentation, 2017, 12(1):P01013.
    [5] JOINER N, ESSER B, FERTIG M, et al. Ceas Space Journal, 2016, 8(4):1.
    [6] CORTESI M, ZBORAY R, ADAMS R, et al. Journal of Instrumentation, 2013, 8(6):C10009.
    [7] ZBORAY R, ADAMS R, CORTESI M, et al. Nuclear Engineering & Design, 2014, 273(2):10.
    [8] WANG Tuo, ZHOU Jianrong, SUN Zhijia, et al. Nucl Phys Rev, 2014, 31(1):69. (in Chinese) (周健荣, 孙志嘉, 吴冲, 等. 原子核物理评论, 2014, 31(1):69.)
    [9] LIU Chuanfeng, ZHOU Xiaojuan, ZHOU Jianrong, et al. Nucl Phys Rev, 2018, 35(1):61. (in Chinese) (刘川凤, 周晓娟, 周健荣, 等. 原子核物理评论, 2018, 35(1):61.)
    [10] DALLA TORRE S. Journal of Instrumentation, 2013, 8(10):C10020.
    [11] KIM J E, KO P, LEE K. Astroparticle, Particle, Space Physics and Detectors for Physics Applications[M]. Singapore:World Scientific, 2012.
    [12] ISRAELASHVILI I, CORTESI M, VARTSKY D, et al. JINST, 2014, 10(3):P03030.
    [13] VARTSKY D, ISRAELASHVILI I, CORTESI M, et al. Nucl Instr and Meth A, 2016, 824(6):240.
    [14] DONG Liyuan, QI Huirong, LI Yuhong, et al. Nucl Phys Rev, 2012, 29(4):379. (in Chinese) (董丽媛, 祁辉荣, 李玉红等. 原子核物理评论, 2012, 29(4):379.)
    [15] WI Kun, QI Huirong, ZHANG Yulian, et al. Nucl Phys Rev, 2015, 32(3):335. (in Chinese) (魏堃, 祁辉荣, 张余炼, 等. 原子核物理评论, 2015, 32(3):335.)
    [16] BRESKIN A, ALON R, CORTESI M, et al. Nucl Instr and Meth A, 2009, 598(1):107.
    [17] LU Liming, ZHOU Xiaojuan, ZHOU Jianrong, et al. NuclPhys Rev, 2018, 35(2):172. (in Chinese) (鲁黎明, 周晓娟, 周健荣, 等. 原子核物理评论, 2018, 35(2):172.)
    [18] SHALEM C, CHECHIK R, BRESKIN A, et al. Nucl Instr and Meth A, 2006, 558(2):475.
    [19] CHECHIK R, BRESKIN A, SHALEM C, et al. Nucl Instr and Meth A, 2004, 535(1):303.
    [20] CORTESI M, ROST S, MITTIG W, et al. Review of Scientific Instruments, 2016, 88(1):123.
    [21] CORTESI M, YURKON J, MITTIG W, et al. Physics, 2015, 10(9):P09020.
    [22] XIE Yuguang, PENG Zhiyuan, LI Genglan. Multilayer Thick GEM (M-THGEM)[R]. Annual Meeting of State Key Laboratory of Particle Detection and Electronics, Beijing, 26 Apr, 2018. (in Chinese) (谢宇广, 彭志远, 李更兰. 多层厚GEM(M-THGEM)研制[R]. 2018年核探测与核电子学国家重点实验室年会, 北京, 2018-04-26.)
    [23] BALL M, ECKSTEIN K, GUNJI T. Journal of Instrumentation, 2014, 9(04):C04025.
  • 加载中
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Article Metrics

Article views(1392) PDF downloads(100) Cited by()

Proportional views

Monte Carlo Simulation on the Novel M-THGEM Detector

doi: 10.11804/NuclPhysRev.36.01.085
Funds:  National Natural Science Foundation of China(11605086,11875163); Natural Science Foundation of Hunan Province, China(2018JJ3422); Research Foundation of Education Bureau of Hunan Province, China(15B205, 18C0461)

Abstract: Compared to THGEM (Thick Gas Electron Multiplier), the novel Multilayer Thick Gaseous Electron Multiplier (M-THGEM) has many advantages, such as continuous avalanche zone, more compact structure, high gain at low pressure and low operating voltage, and easy to make large-area production. In the presented work, two types of the M-THGEM detector (two or three layers) were modeled, and their main principle and performances were also studied by simulation. Two types of the detector were molded and simulated by using the finite element software (ANSYS), and the electric field distribution and nodes information lists were figured out. The effective gain and induced signal from M-THGEM detector at different gas pressures and operating voltages were studied with the Garfield++ package. The simulation results shown that M-THGEM can obtain a stable higher gain around 105 in an environment where has a low pressure even in 200 Torr and within a pure inertia gas such as He. At this condition, the width of the induced signal from the three-layers structure is around 120 ns. Additionally, an asymmetric way of the applied voltage was studied and aim to reduce the efficiency of ion feedback, and our results show that this method is effective.

WEI Xin, WANG Xiaodong, CHENG Kai, DIAO Weizhuo, CHEN Guoxiang, HE Sanjun, LI Tingting, ZHAO Yue, LIU Zheng. Monte Carlo Simulation on the Novel M-THGEM Detector[J]. Nuclear Physics Review, 2019, 36(1): 85-90. doi: 10.11804/NuclPhysRev.36.01.085
Citation: WEI Xin, WANG Xiaodong, CHENG Kai, DIAO Weizhuo, CHEN Guoxiang, HE Sanjun, LI Tingting, ZHAO Yue, LIU Zheng. Monte Carlo Simulation on the Novel M-THGEM Detector[J]. Nuclear Physics Review, 2019, 36(1): 85-90. doi: 10.11804/NuclPhysRev.36.01.085
Reference (23)

Catalog

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return