Interdefect charge exchange in silicon particle detectors at cryogenic temperatures
Silicon particle detectors in the next generation of experiments at the CERN Large Hadron Collider will be exposed to a very challenging radiation environment. The principal obstacle to long-term operation arises from changes in detector doping concentration (N/sub eff/), which lead to an increase i...
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Published in | IEEE transactions on nuclear science Vol. 49; no. 4; pp. 1750 - 1755 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
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New York
IEEE
01.08.2002
The Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
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Abstract | Silicon particle detectors in the next generation of experiments at the CERN Large Hadron Collider will be exposed to a very challenging radiation environment. The principal obstacle to long-term operation arises from changes in detector doping concentration (N/sub eff/), which lead to an increase in the bias required to deplete the detector and hence achieve efficient charge collection. We have previously presented a model of interdefect charge exchange between closely spaced centers in the dense terminal clusters formed by hadron irradiation. This manifestly non-Shockley-Read-Hall (SRH) mechanism leads to a marked increase in carrier generation rate and negative space charge over the SRH prediction. There is currently much interest in the subject of cryogenic detector operation as a means of improving radiation hardness. Our motivation, however, is primarily to investigate our model further by testing its predictions over a range of temperatures. We present measurements of spectra from /sup 241/Am alpha particles and 1064-nm laser pulses as a function of bias between 120 and 290 K. Values of N/sub eff/ and substrate type are extracted from the spectra and compared with the model. The model is implemented in both a commercial finite-element device simulator (ISE-TCAD) and a purpose-built simulation of interdefect charge exchange. Deviations from the model are explored and comments made as to possible future directions for investigation of this difficult problem. |
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AbstractList | Silicon particle detectors in the next generation of experiments at the CERN Large Hadron Collider will be exposed to a very challenging radiation environment. The principal obstacle to long-term operation arises from changes in detector doping concentration (N/eff/), which lead to an increase in the bias required to deplete the detector and hence achieve efficient charge collection. We have previously presented a model of interdefect charge exchange between closely spaced centers in the dense terminal clusters formed by hadron irradiation. This manifestly non-Shockley-Read-Hall (SRH) mechanism leads to a marked increase in carrier generation rate and negative space charge over the SRH prediction. There is currently much interest in the subject of cryogenic detector operation as a means of improving radiation hardness. Our motivation, however, is primarily to investigate our model further by testing its predictions over a range of temperatures. We present measurements of spectra from /241/Am alpha particles and 1064-nm laser pulses as a function of bias between 120 and 290 K. Values of N/eff/ and substrate type are extracted from the spectra and compared with the model. The model is implemented in both a commercial finite-element device simulator (ISE-TCAD) and a purpose-built simulation of interdefect charge exchange. Deviations from the model are explored and comments made as to possible future directions for investigation of this difficult problem. The principal obstacle to long-term operation arises from changes in detector doping concentration (Neff), which lead to an increase in the bias required to deplete the detector and hence achieve efficient charge collection. Silicon particle detectors in the next generation of experiments at the CERN Large Hadron Collider will be exposed to a very challenging radiation environment. The principal obstacle to long-term operation arises from changes in detector doping concentration (N/sub eff/), which lead to an increase in the bias required to deplete the detector and hence achieve efficient charge collection. We have previously presented a model of interdefect charge exchange between closely spaced centers in the dense terminal clusters formed by hadron irradiation. This manifestly non-Shockley-Read-Hall (SRH) mechanism leads to a marked increase in carrier generation rate and negative space charge over the SRH prediction. There is currently much interest in the subject of cryogenic detector operation as a means of improving radiation hardness. Our motivation, however, is primarily to investigate our model further by testing its predictions over a range of temperatures. We present measurements of spectra from /sup 241/Am alpha particles and 1064-nm laser pulses as a function of bias between 120 and 290 K. Values of N/sub eff/ and substrate type are extracted from the spectra and compared with the model. The model is implemented in both a commercial finite-element device simulator (ISE-TCAD) and a purpose-built simulation of interdefect charge exchange. Deviations from the model are explored and comments made as to possible future directions for investigation of this difficult problem. Silicon particle detectors in the next generation of experiments at the CERN Large Hadron Collider will be exposed to a very challenging radiation environment. The principal obstacle to long-term operation arises from changes in detector doping concentration (N sub(eff)), which lead to an increase in the bias required to deplete the detector and hence achieve efficient charge collection. We have previously presented a model of interdefect charge exchange between closely spaced centers in the dense terminal clusters formed by hadron irradiation. This manifestly non-Shockley-Read-Hall (SRH) mechanism leads to a marked increase in carrier generation rate and negative space charge over the SRH prediction. There is currently much interest in the subject of cryogenic detector operation as a means of improving radiation hardness. Our motivation, however, is primarily to investigate our model further by testing its predictions over a range of temperatures. We present measurements of spectra from super(241)Am alpha particles and 1064-nm laser pulses as a function of bias between 120 and 290 K. Values of N sub(eff) and substrate type are extracted from the spectra and compared with the model. The model is implemented in both a commercial finite-element device simulator (ISE-TCAD) and a purpose-built simulation of interdefect charge exchange. Deviations from the model are explored and comments made as to possible future directions for investigation of this difficult problem. |
Author | Santocchia, A. Passeri, D. Moscatelli, F. MacEvoy, B. Hall, G. Bilei, G.M. |
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Cites_doi | 10.1016/0168-9002(96)37410-X 10.1016/0168-9002(87)90532-8 10.1088/0268-1242/2/8/009 10.1103/PhysRev.87.387 10.1063/1.365790 10.1016/S1369-8001(00)00039-1 10.1016/S0168-9002(00)00788-9 10.1109/23.556840 10.1016/S0168-583X(01)00899-0 10.1103/PhysRev.87.835 10.1016/S0921-4526(99)00635-3 10.1016/S0168-9002(00)00450-2 10.1063/1.361816 10.1016/0168-9002(94)01728-X 10.1103/PhysRevLett.72.2939 10.1109/23.960358 |
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References | ref13 ref12 ref15 Lemeilleur (ref2) 1995; A360 Ahmed (ref10) 2001; A457 ref14 Sze (ref16) 1981 ref11 ref17 ref18 ref8 ref7 ref9 ref4 ref3 ref6 ref5 |
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SubjectTerms | Bias Charge exchange Computer simulation Cryogenics Detectors Doping Hadrons Large Hadron Collider Mathematical models Predictive models Pulse measurements Radiation detectors Semiconductor process modeling Silicon Space charge Spectra Temperature |
Title | Interdefect charge exchange in silicon particle detectors at cryogenic temperatures |
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