Secondary discharge studies in single- and multi-GEM structures
Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the abs...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Deisting, Alexander - 1989- [verfasserIn] Garabatos, Chilo [verfasserIn] Gasik, P. [verfasserIn] Baitinger, Daniel [verfasserIn] Berdnikova, A. [verfasserIn] Blidaru, Mihail-Bogdan [verfasserIn] Datz, A. [verfasserIn] Dufter, F. [verfasserIn] Hassan, S. [verfasserIn] Klemenz, T. [verfasserIn] Lautner, L. [verfasserIn] Masciocchi, Silvia [verfasserIn] Mathis, A. [verfasserIn] Negrao De Oliveira, R. A. [verfasserIn] Szabo, A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
23 May 2019 |
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| Schlagwörter: |
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| Anmerkung: |
Gesehen am 20.11.2019 |
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| Umfang: |
13 |
| Übergeordnetes Werk: |
Enthalten in: Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment - Amsterdam : North-Holland Publ. Co., 1984, 937(2019), Seite 168-180 |
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| Übergeordnetes Werk: |
volume:937 ; year:2019 ; pages:168-180 ; extent:13 |
| Links: |
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| DOI / URN: |
10.1016/j.nima.2019.05.057 |
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| Katalog-ID: |
1682260100 |
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| 245 | 1 | 0 | |a Secondary discharge studies in single- and multi-GEM structures |c A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo |
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| 520 | |a Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. | ||
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| 650 | 4 | |a Onset field | |
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10.1016/j.nima.2019.05.057 doi (DE-627)1682260100 (DE-599)KXP1682260100 (OCoLC)1341278450 DE-627 ger DE-627 rda eng Deisting, Alexander 1989- verfasserin (DE-588)1154513815 (DE-627)1015806686 (DE-576)501055851 aut Secondary discharge studies in single- and multi-GEM structures A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo 23 May 2019 13 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Gesehen am 20.11.2019 Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Characteristic charge Decoupling resistor Discharge GEM Onset field Secondary discharge Garabatos, Chilo verfasserin (DE-588)116875688X (DE-627)1032530820 (DE-576)511721412 aut Gasik, P. verfasserin aut Baitinger, Daniel verfasserin (DE-588)120005900X (DE-627)1682258882 aut Berdnikova, A. verfasserin aut Blidaru, Mihail-Bogdan verfasserin (DE-588)1200059212 (DE-627)1682259501 aut Datz, A. verfasserin aut Dufter, F. verfasserin aut Hassan, S. verfasserin aut Klemenz, T. verfasserin aut Lautner, L. verfasserin aut Masciocchi, Silvia verfasserin (DE-588)1154514447 (DE-627)1015807623 (DE-576)176115749 aut Mathis, A. verfasserin aut Negrao De Oliveira, R. A. verfasserin aut Szabo, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Amsterdam : North-Holland Publ. Co., 1984 937(2019), Seite 168-180 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:937 year:2019 pages:168-180 extent:13 https://doi.org/10.1016/j.nima.2019.05.057 Verlag Resolving-System Volltext http://www.sciencedirect.com/science/article/pii/S0168900219307132 Verlag Resolving-System Volltext GBV_USEFLAG_U GBV_ILN_2013 ISIL_DE-16-250 SYSFLAG_1 GBV_KXP 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 AR 937 2019 168-180 13 2013 01 DE-16-250 3543135147 00 --%%-- --%%-- --%%-- --%%-- l01 20-11-19 2013 01 DE-16-250 00 s hd2019 2013 01 DE-16-250 01 s (DE-627)1410508463 wissenschaftlicher Artikel (Zeitschrift) 2013 01 DE-16-250 02 s per_15 2013 01 DE-16-250 03 s s_13 2013 01 DE-16-250 04 p (DE-627)1571056742 Deisting, Alexander 2013 01 DE-16-250 04 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 04 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 04 s pos_1 2013 01 DE-16-250 05 p (DE-627)1682258955 Baitinger, Daniel 2013 01 DE-16-250 05 k (DE-627)1416822720 Extern 2013 01 DE-16-250 05 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 05 s pos_4 2013 01 DE-16-250 06 p (DE-627)1682259536 Blidaru, Mihail-Bogdan 2013 01 DE-16-250 06 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 06 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 06 s pos_6 2013 01 DE-16-250 07 p (DE-627)1585635421 Masciocchi, Silvia 2013 01 DE-16-250 07 k (DE-627)1416822720 Extern 2013 01 DE-16-250 07 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 07 s pos_12 |
| spelling |
10.1016/j.nima.2019.05.057 doi (DE-627)1682260100 (DE-599)KXP1682260100 (OCoLC)1341278450 DE-627 ger DE-627 rda eng Deisting, Alexander 1989- verfasserin (DE-588)1154513815 (DE-627)1015806686 (DE-576)501055851 aut Secondary discharge studies in single- and multi-GEM structures A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo 23 May 2019 13 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Gesehen am 20.11.2019 Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Characteristic charge Decoupling resistor Discharge GEM Onset field Secondary discharge Garabatos, Chilo verfasserin (DE-588)116875688X (DE-627)1032530820 (DE-576)511721412 aut Gasik, P. verfasserin aut Baitinger, Daniel verfasserin (DE-588)120005900X (DE-627)1682258882 aut Berdnikova, A. verfasserin aut Blidaru, Mihail-Bogdan verfasserin (DE-588)1200059212 (DE-627)1682259501 aut Datz, A. verfasserin aut Dufter, F. verfasserin aut Hassan, S. verfasserin aut Klemenz, T. verfasserin aut Lautner, L. verfasserin aut Masciocchi, Silvia verfasserin (DE-588)1154514447 (DE-627)1015807623 (DE-576)176115749 aut Mathis, A. verfasserin aut Negrao De Oliveira, R. A. verfasserin aut Szabo, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Amsterdam : North-Holland Publ. Co., 1984 937(2019), Seite 168-180 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:937 year:2019 pages:168-180 extent:13 https://doi.org/10.1016/j.nima.2019.05.057 Verlag Resolving-System Volltext http://www.sciencedirect.com/science/article/pii/S0168900219307132 Verlag Resolving-System Volltext GBV_USEFLAG_U GBV_ILN_2013 ISIL_DE-16-250 SYSFLAG_1 GBV_KXP 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 AR 937 2019 168-180 13 2013 01 DE-16-250 3543135147 00 --%%-- --%%-- --%%-- --%%-- l01 20-11-19 2013 01 DE-16-250 00 s hd2019 2013 01 DE-16-250 01 s (DE-627)1410508463 wissenschaftlicher Artikel (Zeitschrift) 2013 01 DE-16-250 02 s per_15 2013 01 DE-16-250 03 s s_13 2013 01 DE-16-250 04 p (DE-627)1571056742 Deisting, Alexander 2013 01 DE-16-250 04 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 04 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 04 s pos_1 2013 01 DE-16-250 05 p (DE-627)1682258955 Baitinger, Daniel 2013 01 DE-16-250 05 k (DE-627)1416822720 Extern 2013 01 DE-16-250 05 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 05 s pos_4 2013 01 DE-16-250 06 p (DE-627)1682259536 Blidaru, Mihail-Bogdan 2013 01 DE-16-250 06 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 06 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 06 s pos_6 2013 01 DE-16-250 07 p (DE-627)1585635421 Masciocchi, Silvia 2013 01 DE-16-250 07 k (DE-627)1416822720 Extern 2013 01 DE-16-250 07 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 07 s pos_12 |
| allfields_unstemmed |
10.1016/j.nima.2019.05.057 doi (DE-627)1682260100 (DE-599)KXP1682260100 (OCoLC)1341278450 DE-627 ger DE-627 rda eng Deisting, Alexander 1989- verfasserin (DE-588)1154513815 (DE-627)1015806686 (DE-576)501055851 aut Secondary discharge studies in single- and multi-GEM structures A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo 23 May 2019 13 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Gesehen am 20.11.2019 Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Characteristic charge Decoupling resistor Discharge GEM Onset field Secondary discharge Garabatos, Chilo verfasserin (DE-588)116875688X (DE-627)1032530820 (DE-576)511721412 aut Gasik, P. verfasserin aut Baitinger, Daniel verfasserin (DE-588)120005900X (DE-627)1682258882 aut Berdnikova, A. verfasserin aut Blidaru, Mihail-Bogdan verfasserin (DE-588)1200059212 (DE-627)1682259501 aut Datz, A. verfasserin aut Dufter, F. verfasserin aut Hassan, S. verfasserin aut Klemenz, T. verfasserin aut Lautner, L. verfasserin aut Masciocchi, Silvia verfasserin (DE-588)1154514447 (DE-627)1015807623 (DE-576)176115749 aut Mathis, A. verfasserin aut Negrao De Oliveira, R. A. verfasserin aut Szabo, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Amsterdam : North-Holland Publ. Co., 1984 937(2019), Seite 168-180 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:937 year:2019 pages:168-180 extent:13 https://doi.org/10.1016/j.nima.2019.05.057 Verlag Resolving-System Volltext http://www.sciencedirect.com/science/article/pii/S0168900219307132 Verlag Resolving-System Volltext GBV_USEFLAG_U GBV_ILN_2013 ISIL_DE-16-250 SYSFLAG_1 GBV_KXP 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 AR 937 2019 168-180 13 2013 01 DE-16-250 3543135147 00 --%%-- --%%-- --%%-- --%%-- l01 20-11-19 2013 01 DE-16-250 00 s hd2019 2013 01 DE-16-250 01 s (DE-627)1410508463 wissenschaftlicher Artikel (Zeitschrift) 2013 01 DE-16-250 02 s per_15 2013 01 DE-16-250 03 s s_13 2013 01 DE-16-250 04 p (DE-627)1571056742 Deisting, Alexander 2013 01 DE-16-250 04 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 04 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 04 s pos_1 2013 01 DE-16-250 05 p (DE-627)1682258955 Baitinger, Daniel 2013 01 DE-16-250 05 k (DE-627)1416822720 Extern 2013 01 DE-16-250 05 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 05 s pos_4 2013 01 DE-16-250 06 p (DE-627)1682259536 Blidaru, Mihail-Bogdan 2013 01 DE-16-250 06 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 06 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 06 s pos_6 2013 01 DE-16-250 07 p (DE-627)1585635421 Masciocchi, Silvia 2013 01 DE-16-250 07 k (DE-627)1416822720 Extern 2013 01 DE-16-250 07 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 07 s pos_12 |
| allfieldsGer |
10.1016/j.nima.2019.05.057 doi (DE-627)1682260100 (DE-599)KXP1682260100 (OCoLC)1341278450 DE-627 ger DE-627 rda eng Deisting, Alexander 1989- verfasserin (DE-588)1154513815 (DE-627)1015806686 (DE-576)501055851 aut Secondary discharge studies in single- and multi-GEM structures A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo 23 May 2019 13 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Gesehen am 20.11.2019 Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Characteristic charge Decoupling resistor Discharge GEM Onset field Secondary discharge Garabatos, Chilo verfasserin (DE-588)116875688X (DE-627)1032530820 (DE-576)511721412 aut Gasik, P. verfasserin aut Baitinger, Daniel verfasserin (DE-588)120005900X (DE-627)1682258882 aut Berdnikova, A. verfasserin aut Blidaru, Mihail-Bogdan verfasserin (DE-588)1200059212 (DE-627)1682259501 aut Datz, A. verfasserin aut Dufter, F. verfasserin aut Hassan, S. verfasserin aut Klemenz, T. verfasserin aut Lautner, L. verfasserin aut Masciocchi, Silvia verfasserin (DE-588)1154514447 (DE-627)1015807623 (DE-576)176115749 aut Mathis, A. verfasserin aut Negrao De Oliveira, R. A. verfasserin aut Szabo, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Amsterdam : North-Holland Publ. Co., 1984 937(2019), Seite 168-180 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:937 year:2019 pages:168-180 extent:13 https://doi.org/10.1016/j.nima.2019.05.057 Verlag Resolving-System Volltext http://www.sciencedirect.com/science/article/pii/S0168900219307132 Verlag Resolving-System Volltext GBV_USEFLAG_U GBV_ILN_2013 ISIL_DE-16-250 SYSFLAG_1 GBV_KXP 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 AR 937 2019 168-180 13 2013 01 DE-16-250 3543135147 00 --%%-- --%%-- --%%-- --%%-- l01 20-11-19 2013 01 DE-16-250 00 s hd2019 2013 01 DE-16-250 01 s (DE-627)1410508463 wissenschaftlicher Artikel (Zeitschrift) 2013 01 DE-16-250 02 s per_15 2013 01 DE-16-250 03 s s_13 2013 01 DE-16-250 04 p (DE-627)1571056742 Deisting, Alexander 2013 01 DE-16-250 04 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 04 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 04 s pos_1 2013 01 DE-16-250 05 p (DE-627)1682258955 Baitinger, Daniel 2013 01 DE-16-250 05 k (DE-627)1416822720 Extern 2013 01 DE-16-250 05 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 05 s pos_4 2013 01 DE-16-250 06 p (DE-627)1682259536 Blidaru, Mihail-Bogdan 2013 01 DE-16-250 06 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 06 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 06 s pos_6 2013 01 DE-16-250 07 p (DE-627)1585635421 Masciocchi, Silvia 2013 01 DE-16-250 07 k (DE-627)1416822720 Extern 2013 01 DE-16-250 07 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 07 s pos_12 |
| allfieldsSound |
10.1016/j.nima.2019.05.057 doi (DE-627)1682260100 (DE-599)KXP1682260100 (OCoLC)1341278450 DE-627 ger DE-627 rda eng Deisting, Alexander 1989- verfasserin (DE-588)1154513815 (DE-627)1015806686 (DE-576)501055851 aut Secondary discharge studies in single- and multi-GEM structures A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo 23 May 2019 13 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Gesehen am 20.11.2019 Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Characteristic charge Decoupling resistor Discharge GEM Onset field Secondary discharge Garabatos, Chilo verfasserin (DE-588)116875688X (DE-627)1032530820 (DE-576)511721412 aut Gasik, P. verfasserin aut Baitinger, Daniel verfasserin (DE-588)120005900X (DE-627)1682258882 aut Berdnikova, A. verfasserin aut Blidaru, Mihail-Bogdan verfasserin (DE-588)1200059212 (DE-627)1682259501 aut Datz, A. verfasserin aut Dufter, F. verfasserin aut Hassan, S. verfasserin aut Klemenz, T. verfasserin aut Lautner, L. verfasserin aut Masciocchi, Silvia verfasserin (DE-588)1154514447 (DE-627)1015807623 (DE-576)176115749 aut Mathis, A. verfasserin aut Negrao De Oliveira, R. A. verfasserin aut Szabo, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Amsterdam : North-Holland Publ. Co., 1984 937(2019), Seite 168-180 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:937 year:2019 pages:168-180 extent:13 https://doi.org/10.1016/j.nima.2019.05.057 Verlag Resolving-System Volltext http://www.sciencedirect.com/science/article/pii/S0168900219307132 Verlag Resolving-System Volltext GBV_USEFLAG_U GBV_ILN_2013 ISIL_DE-16-250 SYSFLAG_1 GBV_KXP 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 AR 937 2019 168-180 13 2013 01 DE-16-250 3543135147 00 --%%-- --%%-- --%%-- --%%-- l01 20-11-19 2013 01 DE-16-250 00 s hd2019 2013 01 DE-16-250 01 s (DE-627)1410508463 wissenschaftlicher Artikel (Zeitschrift) 2013 01 DE-16-250 02 s per_15 2013 01 DE-16-250 03 s s_13 2013 01 DE-16-250 04 p (DE-627)1571056742 Deisting, Alexander 2013 01 DE-16-250 04 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 04 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 04 s pos_1 2013 01 DE-16-250 05 p (DE-627)1682258955 Baitinger, Daniel 2013 01 DE-16-250 05 k (DE-627)1416822720 Extern 2013 01 DE-16-250 05 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 05 s pos_4 2013 01 DE-16-250 06 p (DE-627)1682259536 Blidaru, Mihail-Bogdan 2013 01 DE-16-250 06 k (DE-627)1416535136 Physikalisches Institut (PI) 2013 01 DE-16-250 06 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 06 s pos_6 2013 01 DE-16-250 07 p (DE-627)1585635421 Masciocchi, Silvia 2013 01 DE-16-250 07 k (DE-627)1416822720 Extern 2013 01 DE-16-250 07 s (DE-627)1410501914 Verfasser 2013 01 DE-16-250 07 s pos_12 |
| language |
English |
| source |
Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment 937(2019), Seite 168-180 volume:937 year:2019 pages:168-180 extent:13 |
| sourceStr |
Enthalten in Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment 937(2019), Seite 168-180 volume:937 year:2019 pages:168-180 extent:13 |
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Article |
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2013:0 |
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findex.gbv.de |
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2013@01 |
| topic_facet |
Characteristic charge Decoupling resistor Discharge GEM Onset field Secondary discharge |
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2013:hd2019 DE-16-250:hd2019 2013:wissenschaftlicher Artikel (Zeitschrift) DE-16-250:wissenschaftlicher Artikel (Zeitschrift) 2013:per_15 DE-16-250:per_15 2013:s_13 DE-16-250:s_13 2013:Deisting, Alexander DE-16-250:Deisting, Alexander 2013:Physikalisches Institut (PI) DE-16-250:Physikalisches Institut (PI) 2013:Verfasser DE-16-250:Verfasser 2013:pos_1 DE-16-250:pos_1 2013:Baitinger, Daniel DE-16-250:Baitinger, Daniel 2013:Extern DE-16-250:Extern 2013:pos_4 DE-16-250:pos_4 2013:Blidaru, Mihail-Bogdan DE-16-250:Blidaru, Mihail-Bogdan 2013:pos_6 DE-16-250:pos_6 2013:Masciocchi, Silvia DE-16-250:Masciocchi, Silvia 2013:pos_12 DE-16-250:pos_12 |
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Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment |
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Deisting, Alexander @@aut@@ Garabatos, Chilo @@aut@@ Gasik, P. @@aut@@ Baitinger, Daniel @@aut@@ Berdnikova, A. @@aut@@ Blidaru, Mihail-Bogdan @@aut@@ Datz, A. @@aut@@ Dufter, F. @@aut@@ Hassan, S. @@aut@@ Klemenz, T. @@aut@@ Lautner, L. @@aut@@ Masciocchi, Silvia @@aut@@ Mathis, A. @@aut@@ Negrao De Oliveira, R. A. @@aut@@ Szabo, A. @@aut@@ |
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2019-01-01T00:00:00Z |
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266014666 |
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1682260100 |
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englisch |
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Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">23 May 2019</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">13</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">Gesehen am 20.11.2019</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. 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Secondary discharge studies in single- and multi-GEM structures A. Deisting, C. Garabatos, P. Gasik, D. Baitinger, A. Berdnikova, M.B. Blidaru, A. Datz, F. Dufter, S. Hassan, T. Klemenz, L. Lautner, S. Masciocchi, A. Mathis, R.A. Negrao De Oliveira, A. Szabo |
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Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Gesehen am 20.11.2019 |
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Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Gesehen am 20.11.2019 |
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Secondary discharges, which consist of the breakdown of a gap near a GEM foil upon a primary discharge across that GEM, are studied in this work. Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. A mechanism involving the heating of the cathode surface as trigger for secondary discharges is proposed. Gesehen am 20.11.2019 |
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Their main characteristics are the occurrence a few 10μs after the primary, the relatively sharp onset at moderate electric fields across the gap, the absence of increased fields in the system, and their occurrence under both field directions. They can be mitigated using series resistors in the high-voltage connection to the GEM electrode facing towards an anode. The electric field at which the onset of secondary discharges occurs indeed increases with increasing resistance. Discharge propagation from GEM to GEM in a multi-GEM system affects the occurrence probability of secondary discharges in the gaps between neighbouring GEMs. Furthermore, evidence of charges flowing through the gap after the primary discharge are reported. Such currents may or may not lead to a secondary discharge. A characteristic charge, of the order of 1010 electrons, has been measured as the threshold for a primary discharge to be followed by a secondary discharge, and this number slightly depends on the gas composition. 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