Optimization of the electron collection efficiency of a large area MCP-PMT for the JUNO experiment

详细信息    查看全文

• 作者：Lin Chen^a ; ^b ; ^e ; ^{chenlin@opt.cn" class="auth_mail" title="E-mail the corresponding author} ; Jinshou Tian^b ; Chunliang Liu^e ; Yifang Wang^c ; Tianchi Zhao^c ; Hulin Liu^b ; Yonglin Wei^b ; Xiaofeng Sai^b ; Ping Chen^a ; ^b ; Xing Wang^b ; Yu Lu^b ; Dandan Hui^a ; ^b ; Lehui Guo^a ; ^b ; Shulin Liu^c ; Sen Qian^c ; Jingkai Xia^c ; Baojun Yan^c ; Na Zhu^c ; Jianning Sun^d ; Shuguang Si^d ; Dong Li^d ; Xingchao Wang^d ; Guorui Huang^d ; Ming Qi^f
• 关键词：Collection efficiency ; Photomultiplier tube ; Microchannel plate
• 刊名：Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
• 出版年：2016
• 出版时间：11 August 2016
• 年：2016
• 卷：827
• 期：Complete
• 页码：124-130
• 全文大小：2676 K

文摘

A novel large-area (20-inch) photomultiplier tube based on microchannel plate (MCP-PMTs) is proposed for the Jiangmen Underground Neutrino Observatory (JUNO) experiment. Its photoelectron collection efficiency C_e is limited by the MCP open area fraction (A_open). This efficiency is studied as a function of the angular (θ), energy (E) distributions of electrons in the input charge cloud and the potential difference (U) between the PMT photocathode and the MCP input surface, considering secondary electron emission from the MCP input electrode. In CST Studio Suite, Finite Integral Technique and Monte Carlo method are combined to investigate the dependence of C_e on θ, E and U. Results predict that C_e can exceed A_open, and are applied to optimize the structure and operational parameters of the 20-inch MCP-PMT prototype. C_e of the optimized MCP-PMT is expected to reach 81.2%. Finally, the reduction of the penetration depth of the MCP input electrode layer and the deposition of a high secondary electron yield material on the MCP are proposed to further optimize C_e.