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Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2

Low Gain Avalanche Detectors (LGADs) are silicon sensors with a built-in charge multiplica- tion layer providing a gain of typically 10 to 50. Due to the combination of high signal-to-noise ratio and short rise time, thin LGADs provide good time resolutions. LGADs with an active thickness of about 4...

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Autores principales: Lange, J., Carulla, M., Cavallaro, E., Chytka, L., Davis, P.M., Flores, D., Förster, F., Grinstein, S., Hidalgo, S., Komarek, T., Kramberger, G., Mandić, I., Merlos, A., Nozka, L., Pellegrini, G., Quirion, D., Sykora, T.
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: JINST 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1748-0221/12/05/P05003
http://cds.cern.ch/record/2623664
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author Lange, J.
Carulla, M.
Cavallaro, E.
Chytka, L.
Davis, P.M.
Flores, D.
Förster, F.
Grinstein, S.
Hidalgo, S.
Komarek, T.
Kramberger, G.
Mandić, I.
Merlos, A.
Nozka, L.
Pellegrini, G.
Quirion, D.
Sykora, T.
author_facet Lange, J.
Carulla, M.
Cavallaro, E.
Chytka, L.
Davis, P.M.
Flores, D.
Förster, F.
Grinstein, S.
Hidalgo, S.
Komarek, T.
Kramberger, G.
Mandić, I.
Merlos, A.
Nozka, L.
Pellegrini, G.
Quirion, D.
Sykora, T.
author_sort Lange, J.
collection CERN
description Low Gain Avalanche Detectors (LGADs) are silicon sensors with a built-in charge multiplica- tion layer providing a gain of typically 10 to 50. Due to the combination of high signal-to-noise ratio and short rise time, thin LGADs provide good time resolutions. LGADs with an active thickness of about 45 μm were produced at CNM Barcelona. Their gains and time resolutions were studied in beam tests for two different multiplication layer implantation doses, as well as before and after irradiation with neutrons up to 1015 neq/cm2. The gain showed the expected decrease at a fixed voltage for a lower initial implantation dose, as well as for a higher fluence due to effective acceptor removal in the multiplication layer. Time resolutions below 30 ps were obtained at the highest applied voltages for both implantation doses before irradiation. Also after an intermediate fluence of 3 × 1014 neq/cm2, similar values were measured since a higher applicable reverse bias voltage could recover most of the pre-irradiation gain. At 1015 neq/cm2, the time resolution at the maximum applicable voltage of 620 V during the beam test was measured to be 57 ps since the voltage stability was not good enough to compensate for the gain layer loss. The time resolutions were found to follow approximately a universal function of gain for all implantation doses and fluences.
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spelling cern-26236642023-03-14T19:33:59Z doi:10.1088/1748-0221/12/05/P05003 http://cds.cern.ch/record/2623664 eng Lange, J. Carulla, M. Cavallaro, E. Chytka, L. Davis, P.M. Flores, D. Förster, F. Grinstein, S. Hidalgo, S. Komarek, T. Kramberger, G. Mandić, I. Merlos, A. Nozka, L. Pellegrini, G. Quirion, D. Sykora, T. Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2 Detectors and Experimental Techniques 6: Novel high voltage and resistive CMOS sensors Low Gain Avalanche Detectors (LGADs) are silicon sensors with a built-in charge multiplica- tion layer providing a gain of typically 10 to 50. Due to the combination of high signal-to-noise ratio and short rise time, thin LGADs provide good time resolutions. LGADs with an active thickness of about 45 μm were produced at CNM Barcelona. Their gains and time resolutions were studied in beam tests for two different multiplication layer implantation doses, as well as before and after irradiation with neutrons up to 1015 neq/cm2. The gain showed the expected decrease at a fixed voltage for a lower initial implantation dose, as well as for a higher fluence due to effective acceptor removal in the multiplication layer. Time resolutions below 30 ps were obtained at the highest applied voltages for both implantation doses before irradiation. Also after an intermediate fluence of 3 × 1014 neq/cm2, similar values were measured since a higher applicable reverse bias voltage could recover most of the pre-irradiation gain. At 1015 neq/cm2, the time resolution at the maximum applicable voltage of 620 V during the beam test was measured to be 57 ps since the voltage stability was not good enough to compensate for the gain layer loss. The time resolutions were found to follow approximately a universal function of gain for all implantation doses and fluences. Low Gain Avalanche Detectors (LGADs) are silicon sensors with a built-in charge multiplication layer providing a gain of typically 10 to 50. Due to the combination of high signal-to-noise ratio and short rise time, thin LGADs provide good time resolutions. LGADs with an active thickness of about 45 μm were produced at CNM Barcelona. Their gains and time resolutions were studied in beam tests for two different multiplication layer implantation doses, as well as before and after irradiation with neutrons up to 10(15) n(eq)/cm(2). The gain showed the expected decrease at a fixed voltage for a lower initial implantation dose, as well as for a higher fluence due to effective acceptor removal in the multiplication layer. Time resolutions below 30 ps were obtained at the highest applied voltages for both implantation doses before irradiation. Also after an intermediate fluence of 3×10(14) n(eq)/cm(2), similar values were measured since a higher applicable reverse bias voltage could recover most of the pre-irradiation gain. At 10(15) n(eq)/cm(2), the time resolution at the maximum applicable voltage of 620 V during the beam test was measured to be 57 ps since the voltage stability was not good enough to compensate for the gain layer loss. The time resolutions were found to follow approximately a universal function of gain for all implantation doses and fluences. Low Gain Avalanche Detectors (LGADs) are silicon sensors with a built-in charge multiplication layer providing a gain of typically 10 to 50. Due to the combination of high signal-to-noise ratio and short rise time, thin LGADs provide good time resolutions. LGADs with an active thickness of about 45 $\mu$m were produced at CNM Barcelona. Their gains and time resolutions were studied in beam tests for two different multiplication layer implantation doses, as well as before and after irradiation with neutrons up to $10^{15}$ n$_{eq}$/cm$^2$. The gain showed the expected decrease at a fixed voltage for a lower initial implantation dose, as well as for a higher fluence due to effective acceptor removal in the multiplication layer. Time resolutions below 30 ps were obtained at the highest applied voltages for both implantation doses before irradiation. Also after an intermediate fluence of $3\times10^{14}$ n$_{eq}$/cm$^2$, similar values were measured since a higher applicable reverse bias voltage could recover most of the pre-irradiation gain. At $10^{15}$ n$_{eq}$/cm$^2$, the time resolution at the maximum applicable voltage of 620 V during the beam test was measured to be 57 ps since the voltage stability was not good enough to compensate for the gain layer loss. The time resolutions were found to follow approximately a universal function of gain for all implantation doses and fluences. info:eu-repo/grantAgreement/EC/FP7/654168 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/2623664 JINST JINST, 05 (2017) pp. P05003 2017-05-06
spellingShingle Detectors and Experimental Techniques
6: Novel high voltage and resistive CMOS sensors
Lange, J.
Carulla, M.
Cavallaro, E.
Chytka, L.
Davis, P.M.
Flores, D.
Förster, F.
Grinstein, S.
Hidalgo, S.
Komarek, T.
Kramberger, G.
Mandić, I.
Merlos, A.
Nozka, L.
Pellegrini, G.
Quirion, D.
Sykora, T.
Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2
title Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2
title_full Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2
title_fullStr Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2
title_full_unstemmed Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2
title_short Gain and time resolution of 45 μm thin Low Gain Avalanche Detectors before and after irradiation up to a fluence of 1015 neq/cm2
title_sort gain and time resolution of 45 μm thin low gain avalanche detectors before and after irradiation up to a fluence of 1015 neq/cm2
topic Detectors and Experimental Techniques
6: Novel high voltage and resistive CMOS sensors
url https://dx.doi.org/10.1088/1748-0221/12/05/P05003
http://cds.cern.ch/record/2623664
http://cds.cern.ch/record/2623664
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