The operation and performance of Current Injected Detector (CID)

被引:4
作者
Eremin, V.
Harkonen, J.
Luukka, P. [1 ]
Li, Z.
Verbitskaya, E.
Vayrynen, S.
Kassamakov, I.
机构
[1] Univ Helsinki, Helsinki Inst Phys, FIN-00014 Helsinki, Finland
[2] Russian Acad Sci, AF Ioffe Physicotech Inst, St Petersburg 194021, Russia
[3] Brookhaven Natl Lab, Upton, NY 11973 USA
[4] Univ Helsinki, Accelerator Lab, FIN-00014 Helsinki, Finland
基金
俄罗斯基础研究基金会; 芬兰科学院;
关键词
Current Injected Detector (CID); radiation hardness; semiconductor detector;
D O I
10.1016/j.nima.2007.08.003
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
Radiation hardness up to 1 x 10(16) cm(-2) is required in the future high-energy physics experiments. This is well beyond the radiation tolerance of even the most advanced semiconductor detectors fabricated by commonly adopted technologies. The Current Injected Detector (CID) is a device in which the current is limited by the space charge, which originates from injected carriers trapped by the deep levels. This induces a stable electric field through the entire detector bulk regardless of the irradiation fluence the detector has been exposed to. The steady state density of the trapped charge is defined by the balance between the trapping and emission rates of charge carriers (detrapping). Thus, the amount of charge injection needed for electric field stabilization depends on the temperature. The CID mode has a new specific feature which limits the maximum operational voltage. It is connected with the space charge density saturation and the sharp current rising at the threshold voltage V-T. The value Of VT is proportional to the irradiation fluence and it increases with respect to the irradiation fluence extending the range of the operation voltage. (C) 2007 Elsevier B.V. All rights reserved.
引用
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页码:356 / 360
页数:5
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