Study on the transit time spread characteristic of 20-in. hybrid photomultiplier tube used for high-energy particle detection

According to the requirements of high-energy particle detection for a large photocathode detection surface, low transit time spread (TTS), and low-cost photomultiplier tube (PMT), a kind of 20-in. hybrid large-area PMT based on the silicon (Si) electron multiplier array was designed and optimized. T...

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Bibliographic Details
Main Authors: Chen, P. (Author), Gao, G. (Author), Guo, L. (Author), He, K. (Author), Ji, C. (Author), Liu, H. (Author), Shen, T. (Author), Tian, J. (Author), Wang, X. (Author), Xin, L. (Author), Xue, Y. (Author)
Format: Article
Language:English
Published: American Institute of Physics Inc. 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02431nam a2200445Ia 4500
001 10.1063-5.0087552
008 220425s2022 CNT 000 0 und d
020 |a 21583226 (ISSN) 
245 1 0 |a Study on the transit time spread characteristic of 20-in. hybrid photomultiplier tube used for high-energy particle detection 
260 0 |b American Institute of Physics Inc.  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1063/5.0087552 
520 3 |a According to the requirements of high-energy particle detection for a large photocathode detection surface, low transit time spread (TTS), and low-cost photomultiplier tube (PMT), a kind of 20-in. hybrid large-area PMT based on the silicon (Si) electron multiplier array was designed and optimized. This study tracked the trajectories of photoelectrons from the photocathode to the silicon electron multiplier array based on the Monte Carlo and finite-integral method. The critical effects on the TTS characteristic of the large-area PMT, including the focusing electrode structure, glass shell structure, different potential differences, and relative distance from the photocathode vertex to the silicon electron multiplier array, were studied in detail. After optimizing the structure of the glass shell, the 20-in. hybrid PMT based on the ultra-small Si electron multiplier array with 40 mm collection diameter can achieve an excellent TTS of about 1.87 ns from the photocathode to the Si electron multiplier array at a collection potential difference of 2000 V. © 2022 Author(s). 
650 0 4 |a Critical effects 
650 0 4 |a Electrode structure 
650 0 4 |a Electrons 
650 0 4 |a Finite integral method 
650 0 4 |a Glass 
650 0 4 |a High-energy particles 
650 0 4 |a Hybrid photomultiplier tubes 
650 0 4 |a Low-costs 
650 0 4 |a Monte Carlo methods 
650 0 4 |a Particles detection 
650 0 4 |a Photocathodes 
650 0 4 |a Photomultipliers 
650 0 4 |a Potential difference 
650 0 4 |a Shell structure 
650 0 4 |a Silicon 
650 0 4 |a Transit time spread 
700 1 |a Chen, P.  |e author 
700 1 |a Gao, G.  |e author 
700 1 |a Guo, L.  |e author 
700 1 |a He, K.  |e author 
700 1 |a Ji, C.  |e author 
700 1 |a Liu, H.  |e author 
700 1 |a Shen, T.  |e author 
700 1 |a Tian, J.  |e author 
700 1 |a Wang, X.  |e author 
700 1 |a Xin, L.  |e author 
700 1 |a Xue, Y.  |e author 
773 |t AIP Advances