A compensated design of the LGAD gain layer
In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local a...
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| Autor*in: |
Sola, V. [verfasserIn] Arcidiacono, R. [verfasserIn] Asenov, P. [verfasserIn] Borghi, G. [verfasserIn] Boscardin, M. [verfasserIn] Cartiglia, N. [verfasserIn] Vignali, M. Centis [verfasserIn] Croci, T. [verfasserIn] Ferrero, M. [verfasserIn] Fondacci, A. [verfasserIn] Gioachin, G. [verfasserIn] Giordanengo, S. [verfasserIn] Lantieri, L. [verfasserIn] Mandurrino, M. [verfasserIn] Menzio, L. [verfasserIn] Monaco, V. [verfasserIn] Morozzi, A. [verfasserIn] Moscatelli, F. [verfasserIn] Passeri, D. [verfasserIn] Pastrone, N. [verfasserIn] Paternoster, G. [verfasserIn] Siviero, F. [verfasserIn] Staiano, A. [verfasserIn] Tornago, M. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Nuclear instruments & methods in physics research / A - Amsterdam : North-Holland Publ. Co., 1984, 1040 |
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| Übergeordnetes Werk: |
volume:1040 |
| DOI / URN: |
10.1016/j.nima.2022.167232 |
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| Katalog-ID: |
ELV008376395 |
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| 100 | 1 | |a Sola, V. |e verfasserin |0 (orcid)0000-0001-6288-951X |4 aut | |
| 245 | 1 | 0 | |a A compensated design of the LGAD gain layer |
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| 520 | |a In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . | ||
| 650 | 4 | |a Silicon sensor | |
| 650 | 4 | |a LGAD | |
| 650 | 4 | |a Compensation | |
| 650 | 4 | |a Compensated LGAD | |
| 650 | 4 | |a Gain layer | |
| 650 | 4 | |a 4D tracking | |
| 650 | 4 | |a Radiation hardness | |
| 700 | 1 | |a Arcidiacono, R. |e verfasserin |4 aut | |
| 700 | 1 | |a Asenov, P. |e verfasserin |0 (orcid)0000-0003-2379-9903 |4 aut | |
| 700 | 1 | |a Borghi, G. |e verfasserin |0 (orcid)0000-0001-8488-4728 |4 aut | |
| 700 | 1 | |a Boscardin, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Cartiglia, N. |e verfasserin |4 aut | |
| 700 | 1 | |a Vignali, M. Centis |e verfasserin |0 (orcid)0000-0002-4177-9087 |4 aut | |
| 700 | 1 | |a Croci, T. |e verfasserin |0 (orcid)0000-0001-5246-0269 |4 aut | |
| 700 | 1 | |a Ferrero, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Fondacci, A. |e verfasserin |0 (orcid)0000-0002-6131-7728 |4 aut | |
| 700 | 1 | |a Gioachin, G. |e verfasserin |4 aut | |
| 700 | 1 | |a Giordanengo, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Lantieri, L. |e verfasserin |0 (orcid)0000-0003-1329-5293 |4 aut | |
| 700 | 1 | |a Mandurrino, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Menzio, L. |e verfasserin |0 (orcid)0000-0002-9697-5608 |4 aut | |
| 700 | 1 | |a Monaco, V. |e verfasserin |4 aut | |
| 700 | 1 | |a Morozzi, A. |e verfasserin |0 (orcid)0000-0003-1611-5024 |4 aut | |
| 700 | 1 | |a Moscatelli, F. |e verfasserin |4 aut | |
| 700 | 1 | |a Passeri, D. |e verfasserin |0 (orcid)0000-0001-5322-2414 |4 aut | |
| 700 | 1 | |a Pastrone, N. |e verfasserin |4 aut | |
| 700 | 1 | |a Paternoster, G. |e verfasserin |4 aut | |
| 700 | 1 | |a Siviero, F. |e verfasserin |0 (orcid)0000-0002-4427-4076 |4 aut | |
| 700 | 1 | |a Staiano, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Tornago, M. |e verfasserin |0 (orcid)0000-0001-6768-1056 |4 aut | |
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10.1016/j.nima.2022.167232 doi (DE-627)ELV008376395 (ELSEVIER)S0168-9002(22)00586-1 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Sola, V. verfasserin (orcid)0000-0001-6288-951X aut A compensated design of the LGAD gain layer 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . Silicon sensor LGAD Compensation Compensated LGAD Gain layer 4D tracking Radiation hardness Arcidiacono, R. verfasserin aut Asenov, P. verfasserin (orcid)0000-0003-2379-9903 aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Boscardin, M. verfasserin aut Cartiglia, N. verfasserin aut Vignali, M. Centis verfasserin (orcid)0000-0002-4177-9087 aut Croci, T. verfasserin (orcid)0000-0001-5246-0269 aut Ferrero, M. verfasserin aut Fondacci, A. verfasserin (orcid)0000-0002-6131-7728 aut Gioachin, G. verfasserin aut Giordanengo, S. verfasserin aut Lantieri, L. verfasserin (orcid)0000-0003-1329-5293 aut Mandurrino, M. verfasserin aut Menzio, L. verfasserin (orcid)0000-0002-9697-5608 aut Monaco, V. verfasserin aut Morozzi, A. verfasserin (orcid)0000-0003-1611-5024 aut Moscatelli, F. verfasserin aut Passeri, D. verfasserin (orcid)0000-0001-5322-2414 aut Pastrone, N. verfasserin aut Paternoster, G. verfasserin aut Siviero, F. verfasserin (orcid)0000-0002-4427-4076 aut Staiano, A. verfasserin aut Tornago, M. verfasserin (orcid)0000-0001-6768-1056 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1040 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1040 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 1040 |
| spelling |
10.1016/j.nima.2022.167232 doi (DE-627)ELV008376395 (ELSEVIER)S0168-9002(22)00586-1 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Sola, V. verfasserin (orcid)0000-0001-6288-951X aut A compensated design of the LGAD gain layer 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . Silicon sensor LGAD Compensation Compensated LGAD Gain layer 4D tracking Radiation hardness Arcidiacono, R. verfasserin aut Asenov, P. verfasserin (orcid)0000-0003-2379-9903 aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Boscardin, M. verfasserin aut Cartiglia, N. verfasserin aut Vignali, M. Centis verfasserin (orcid)0000-0002-4177-9087 aut Croci, T. verfasserin (orcid)0000-0001-5246-0269 aut Ferrero, M. verfasserin aut Fondacci, A. verfasserin (orcid)0000-0002-6131-7728 aut Gioachin, G. verfasserin aut Giordanengo, S. verfasserin aut Lantieri, L. verfasserin (orcid)0000-0003-1329-5293 aut Mandurrino, M. verfasserin aut Menzio, L. verfasserin (orcid)0000-0002-9697-5608 aut Monaco, V. verfasserin aut Morozzi, A. verfasserin (orcid)0000-0003-1611-5024 aut Moscatelli, F. verfasserin aut Passeri, D. verfasserin (orcid)0000-0001-5322-2414 aut Pastrone, N. verfasserin aut Paternoster, G. verfasserin aut Siviero, F. verfasserin (orcid)0000-0002-4427-4076 aut Staiano, A. verfasserin aut Tornago, M. verfasserin (orcid)0000-0001-6768-1056 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1040 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1040 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 1040 |
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10.1016/j.nima.2022.167232 doi (DE-627)ELV008376395 (ELSEVIER)S0168-9002(22)00586-1 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Sola, V. verfasserin (orcid)0000-0001-6288-951X aut A compensated design of the LGAD gain layer 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . Silicon sensor LGAD Compensation Compensated LGAD Gain layer 4D tracking Radiation hardness Arcidiacono, R. verfasserin aut Asenov, P. verfasserin (orcid)0000-0003-2379-9903 aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Boscardin, M. verfasserin aut Cartiglia, N. verfasserin aut Vignali, M. Centis verfasserin (orcid)0000-0002-4177-9087 aut Croci, T. verfasserin (orcid)0000-0001-5246-0269 aut Ferrero, M. verfasserin aut Fondacci, A. verfasserin (orcid)0000-0002-6131-7728 aut Gioachin, G. verfasserin aut Giordanengo, S. verfasserin aut Lantieri, L. verfasserin (orcid)0000-0003-1329-5293 aut Mandurrino, M. verfasserin aut Menzio, L. verfasserin (orcid)0000-0002-9697-5608 aut Monaco, V. verfasserin aut Morozzi, A. verfasserin (orcid)0000-0003-1611-5024 aut Moscatelli, F. verfasserin aut Passeri, D. verfasserin (orcid)0000-0001-5322-2414 aut Pastrone, N. verfasserin aut Paternoster, G. verfasserin aut Siviero, F. verfasserin (orcid)0000-0002-4427-4076 aut Staiano, A. verfasserin aut Tornago, M. verfasserin (orcid)0000-0001-6768-1056 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1040 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1040 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 1040 |
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10.1016/j.nima.2022.167232 doi (DE-627)ELV008376395 (ELSEVIER)S0168-9002(22)00586-1 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Sola, V. verfasserin (orcid)0000-0001-6288-951X aut A compensated design of the LGAD gain layer 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . Silicon sensor LGAD Compensation Compensated LGAD Gain layer 4D tracking Radiation hardness Arcidiacono, R. verfasserin aut Asenov, P. verfasserin (orcid)0000-0003-2379-9903 aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Boscardin, M. verfasserin aut Cartiglia, N. verfasserin aut Vignali, M. Centis verfasserin (orcid)0000-0002-4177-9087 aut Croci, T. verfasserin (orcid)0000-0001-5246-0269 aut Ferrero, M. verfasserin aut Fondacci, A. verfasserin (orcid)0000-0002-6131-7728 aut Gioachin, G. verfasserin aut Giordanengo, S. verfasserin aut Lantieri, L. verfasserin (orcid)0000-0003-1329-5293 aut Mandurrino, M. verfasserin aut Menzio, L. verfasserin (orcid)0000-0002-9697-5608 aut Monaco, V. verfasserin aut Morozzi, A. verfasserin (orcid)0000-0003-1611-5024 aut Moscatelli, F. verfasserin aut Passeri, D. verfasserin (orcid)0000-0001-5322-2414 aut Pastrone, N. verfasserin aut Paternoster, G. verfasserin aut Siviero, F. verfasserin (orcid)0000-0002-4427-4076 aut Staiano, A. verfasserin aut Tornago, M. verfasserin (orcid)0000-0001-6768-1056 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1040 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1040 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 1040 |
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10.1016/j.nima.2022.167232 doi (DE-627)ELV008376395 (ELSEVIER)S0168-9002(22)00586-1 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Sola, V. verfasserin (orcid)0000-0001-6288-951X aut A compensated design of the LGAD gain layer 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . Silicon sensor LGAD Compensation Compensated LGAD Gain layer 4D tracking Radiation hardness Arcidiacono, R. verfasserin aut Asenov, P. verfasserin (orcid)0000-0003-2379-9903 aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Boscardin, M. verfasserin aut Cartiglia, N. verfasserin aut Vignali, M. Centis verfasserin (orcid)0000-0002-4177-9087 aut Croci, T. verfasserin (orcid)0000-0001-5246-0269 aut Ferrero, M. verfasserin aut Fondacci, A. verfasserin (orcid)0000-0002-6131-7728 aut Gioachin, G. verfasserin aut Giordanengo, S. verfasserin aut Lantieri, L. verfasserin (orcid)0000-0003-1329-5293 aut Mandurrino, M. verfasserin aut Menzio, L. verfasserin (orcid)0000-0002-9697-5608 aut Monaco, V. verfasserin aut Morozzi, A. verfasserin (orcid)0000-0003-1611-5024 aut Moscatelli, F. verfasserin aut Passeri, D. verfasserin (orcid)0000-0001-5322-2414 aut Pastrone, N. verfasserin aut Paternoster, G. verfasserin aut Siviero, F. verfasserin (orcid)0000-0002-4427-4076 aut Staiano, A. verfasserin aut Tornago, M. verfasserin (orcid)0000-0001-6768-1056 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1040 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1040 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 1040 |
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Silicon sensor LGAD Compensation Compensated LGAD Gain layer 4D tracking Radiation hardness |
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Sola, V. @@aut@@ Arcidiacono, R. @@aut@@ Asenov, P. @@aut@@ Borghi, G. @@aut@@ Boscardin, M. @@aut@@ Cartiglia, N. @@aut@@ Vignali, M. Centis @@aut@@ Croci, T. @@aut@@ Ferrero, M. @@aut@@ Fondacci, A. @@aut@@ Gioachin, G. @@aut@@ Giordanengo, S. @@aut@@ Lantieri, L. @@aut@@ Mandurrino, M. @@aut@@ Menzio, L. @@aut@@ Monaco, V. @@aut@@ Morozzi, A. @@aut@@ Moscatelli, F. @@aut@@ Passeri, D. @@aut@@ Pastrone, N. @@aut@@ Paternoster, G. @@aut@@ Siviero, F. @@aut@@ Staiano, A. @@aut@@ Tornago, M. @@aut@@ |
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a compensated design of the lgad gain layer |
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A compensated design of the LGAD gain layer |
| abstract |
In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . |
| abstractGer |
In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . |
| abstract_unstemmed |
In this contribution, we present an innovative design of the Low-Gain Avalanche Diode (LGAD) gain layer, the p + implant responsible for the local and controlled signal multiplication. In the standard LGAD design, the gain layer is obtained by implanting ∼ 5E16/cm 3 atoms of an acceptor material, typically Boron or Gallium, in the region below the n + + electrode. In our design, we aim at designing a gain layer resulting from the overlap of a p + and an n + implants: the difference between acceptor and donor doping will result in an effective concentration of about 5E16/cm 3 , similar to standard LGADs. At present, the gain mechanism of LGAD sensors under irradiation is maintained up to a fluence of ∼ 1–2E15/cm 2 , and then it is lost due to the acceptor removal mechanism. The new design will be more resilient to radiation, as both acceptor and donor atoms will undergo removal with irradiation, but their difference will maintain constant. The compensated design will empower the 4D tracking ability typical of the LGAD sensors well above 1E16/cm 2 . |
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| title_short |
A compensated design of the LGAD gain layer |
| remote_bool |
true |
| author2 |
Arcidiacono, R. Asenov, P. Borghi, G. Boscardin, M. Cartiglia, N. Vignali, M. Centis Croci, T. Ferrero, M. Fondacci, A. Gioachin, G. Giordanengo, S. Lantieri, L. Mandurrino, M. Menzio, L. Monaco, V. Morozzi, A. Moscatelli, F. Passeri, D. Pastrone, N. Paternoster, G. Siviero, F. Staiano, A. Tornago, M. |
| author2Str |
Arcidiacono, R. Asenov, P. Borghi, G. Boscardin, M. Cartiglia, N. Vignali, M. Centis Croci, T. Ferrero, M. Fondacci, A. Gioachin, G. Giordanengo, S. Lantieri, L. Mandurrino, M. Menzio, L. Monaco, V. Morozzi, A. Moscatelli, F. Passeri, D. Pastrone, N. Paternoster, G. Siviero, F. Staiano, A. Tornago, M. |
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266014666 |
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c |
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false |
| hochschulschrift_bool |
false |
| doi_str |
10.1016/j.nima.2022.167232 |
| up_date |
2024-07-06T19:29:28.009Z |
| _version_ |
1803859177516302336 |
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|
| score |
7.400977 |