Particle identification system for the Super Charm–Tau Factory at Novosibirsk
The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Barnyakov, A.Yu. [verfasserIn] Barnyakov, M.Yu. [verfasserIn] Boborovnikov, V.S. [verfasserIn] Buzykaev, A.R. [verfasserIn] Bykov, A.V. [verfasserIn] Danilyuk, A.F. [verfasserIn] Katcin, A.A. [verfasserIn] Kononov, S.A. [verfasserIn] Korda, D.V. [verfasserIn] Kravchenko, E.A. [verfasserIn] Kuyanov, I.A. [verfasserIn] Onuchin, A.P. [verfasserIn] Ovtin, I.V. [verfasserIn] Podgornov, N.A. [verfasserIn] Porosev, V.V. [verfasserIn] Razuvaev, G.P. [verfasserIn] Rodiakin, V.A. [verfasserIn] Todyshev, K.Yu. [verfasserIn] Vorobyev, V.S. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2019 |
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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, 958 |
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| Übergeordnetes Werk: |
volume:958 |
| DOI / URN: |
10.1016/j.nima.2019.162352 |
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| Katalog-ID: |
ELV003681157 |
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| 245 | 1 | 0 | |a Particle identification system for the Super Charm–Tau Factory at Novosibirsk |
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| 520 | |a The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. | ||
| 650 | 4 | |a Aerogel | |
| 650 | 4 | |a RICH | |
| 650 | 4 | |a ToF | |
| 650 | 4 | |a TOP | |
| 650 | 4 | |a Shifter | |
| 650 | 4 | |a ASHIPH | |
| 650 | 4 | |a PID system | |
| 650 | 4 | |a Particle separation | |
| 700 | 1 | |a Barnyakov, M.Yu. |e verfasserin |4 aut | |
| 700 | 1 | |a Boborovnikov, V.S. |e verfasserin |4 aut | |
| 700 | 1 | |a Buzykaev, A.R. |e verfasserin |4 aut | |
| 700 | 1 | |a Bykov, A.V. |e verfasserin |4 aut | |
| 700 | 1 | |a Danilyuk, A.F. |e verfasserin |4 aut | |
| 700 | 1 | |a Katcin, A.A. |e verfasserin |4 aut | |
| 700 | 1 | |a Kononov, S.A. |e verfasserin |4 aut | |
| 700 | 1 | |a Korda, D.V. |e verfasserin |4 aut | |
| 700 | 1 | |a Kravchenko, E.A. |e verfasserin |4 aut | |
| 700 | 1 | |a Kuyanov, I.A. |e verfasserin |4 aut | |
| 700 | 1 | |a Onuchin, A.P. |e verfasserin |4 aut | |
| 700 | 1 | |a Ovtin, I.V. |e verfasserin |4 aut | |
| 700 | 1 | |a Podgornov, N.A. |e verfasserin |4 aut | |
| 700 | 1 | |a Porosev, V.V. |e verfasserin |4 aut | |
| 700 | 1 | |a Razuvaev, G.P. |e verfasserin |4 aut | |
| 700 | 1 | |a Rodiakin, V.A. |e verfasserin |4 aut | |
| 700 | 1 | |a Todyshev, K.Yu. |e verfasserin |4 aut | |
| 700 | 1 | |a Vorobyev, V.S. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Nuclear instruments & methods in physics research / A |d Amsterdam : North-Holland Publ. Co., 1984 |g 958 |h Online-Ressource |w (DE-627)266014666 |w (DE-600)1466532-3 |w (DE-576)074959743 |x 0168-9002 |7 nnns |
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10.1016/j.nima.2019.162352 doi (DE-627)ELV003681157 (ELSEVIER)S0168-9002(19)30932-5 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Barnyakov, A.Yu. verfasserin aut Particle identification system for the Super Charm–Tau Factory at Novosibirsk 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. Aerogel RICH ToF TOP Shifter ASHIPH PID system Particle separation Barnyakov, M.Yu. verfasserin aut Boborovnikov, V.S. verfasserin aut Buzykaev, A.R. verfasserin aut Bykov, A.V. verfasserin aut Danilyuk, A.F. verfasserin aut Katcin, A.A. verfasserin aut Kononov, S.A. verfasserin aut Korda, D.V. verfasserin aut Kravchenko, E.A. verfasserin aut Kuyanov, I.A. verfasserin aut Onuchin, A.P. verfasserin aut Ovtin, I.V. verfasserin aut Podgornov, N.A. verfasserin aut Porosev, V.V. verfasserin aut Razuvaev, G.P. verfasserin aut Rodiakin, V.A. verfasserin aut Todyshev, K.Yu. verfasserin aut Vorobyev, V.S. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 958 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:958 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 33.07 Spektroskopie 33.40 Kernphysik AR 958 |
| spelling |
10.1016/j.nima.2019.162352 doi (DE-627)ELV003681157 (ELSEVIER)S0168-9002(19)30932-5 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Barnyakov, A.Yu. verfasserin aut Particle identification system for the Super Charm–Tau Factory at Novosibirsk 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. Aerogel RICH ToF TOP Shifter ASHIPH PID system Particle separation Barnyakov, M.Yu. verfasserin aut Boborovnikov, V.S. verfasserin aut Buzykaev, A.R. verfasserin aut Bykov, A.V. verfasserin aut Danilyuk, A.F. verfasserin aut Katcin, A.A. verfasserin aut Kononov, S.A. verfasserin aut Korda, D.V. verfasserin aut Kravchenko, E.A. verfasserin aut Kuyanov, I.A. verfasserin aut Onuchin, A.P. verfasserin aut Ovtin, I.V. verfasserin aut Podgornov, N.A. verfasserin aut Porosev, V.V. verfasserin aut Razuvaev, G.P. verfasserin aut Rodiakin, V.A. verfasserin aut Todyshev, K.Yu. verfasserin aut Vorobyev, V.S. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 958 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:958 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 33.07 Spektroskopie 33.40 Kernphysik AR 958 |
| allfields_unstemmed |
10.1016/j.nima.2019.162352 doi (DE-627)ELV003681157 (ELSEVIER)S0168-9002(19)30932-5 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Barnyakov, A.Yu. verfasserin aut Particle identification system for the Super Charm–Tau Factory at Novosibirsk 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. Aerogel RICH ToF TOP Shifter ASHIPH PID system Particle separation Barnyakov, M.Yu. verfasserin aut Boborovnikov, V.S. verfasserin aut Buzykaev, A.R. verfasserin aut Bykov, A.V. verfasserin aut Danilyuk, A.F. verfasserin aut Katcin, A.A. verfasserin aut Kononov, S.A. verfasserin aut Korda, D.V. verfasserin aut Kravchenko, E.A. verfasserin aut Kuyanov, I.A. verfasserin aut Onuchin, A.P. verfasserin aut Ovtin, I.V. verfasserin aut Podgornov, N.A. verfasserin aut Porosev, V.V. verfasserin aut Razuvaev, G.P. verfasserin aut Rodiakin, V.A. verfasserin aut Todyshev, K.Yu. verfasserin aut Vorobyev, V.S. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 958 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:958 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 33.07 Spektroskopie 33.40 Kernphysik AR 958 |
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10.1016/j.nima.2019.162352 doi (DE-627)ELV003681157 (ELSEVIER)S0168-9002(19)30932-5 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Barnyakov, A.Yu. verfasserin aut Particle identification system for the Super Charm–Tau Factory at Novosibirsk 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. Aerogel RICH ToF TOP Shifter ASHIPH PID system Particle separation Barnyakov, M.Yu. verfasserin aut Boborovnikov, V.S. verfasserin aut Buzykaev, A.R. verfasserin aut Bykov, A.V. verfasserin aut Danilyuk, A.F. verfasserin aut Katcin, A.A. verfasserin aut Kononov, S.A. verfasserin aut Korda, D.V. verfasserin aut Kravchenko, E.A. verfasserin aut Kuyanov, I.A. verfasserin aut Onuchin, A.P. verfasserin aut Ovtin, I.V. verfasserin aut Podgornov, N.A. verfasserin aut Porosev, V.V. verfasserin aut Razuvaev, G.P. verfasserin aut Rodiakin, V.A. verfasserin aut Todyshev, K.Yu. verfasserin aut Vorobyev, V.S. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 958 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:958 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 33.07 Spektroskopie 33.40 Kernphysik AR 958 |
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10.1016/j.nima.2019.162352 doi (DE-627)ELV003681157 (ELSEVIER)S0168-9002(19)30932-5 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Barnyakov, A.Yu. verfasserin aut Particle identification system for the Super Charm–Tau Factory at Novosibirsk 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. Aerogel RICH ToF TOP Shifter ASHIPH PID system Particle separation Barnyakov, M.Yu. verfasserin aut Boborovnikov, V.S. verfasserin aut Buzykaev, A.R. verfasserin aut Bykov, A.V. verfasserin aut Danilyuk, A.F. verfasserin aut Katcin, A.A. verfasserin aut Kononov, S.A. verfasserin aut Korda, D.V. verfasserin aut Kravchenko, E.A. verfasserin aut Kuyanov, I.A. verfasserin aut Onuchin, A.P. verfasserin aut Ovtin, I.V. verfasserin aut Podgornov, N.A. verfasserin aut Porosev, V.V. verfasserin aut Razuvaev, G.P. verfasserin aut Rodiakin, V.A. verfasserin aut Todyshev, K.Yu. verfasserin aut Vorobyev, V.S. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 958 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:958 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 33.07 Spektroskopie 33.40 Kernphysik AR 958 |
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Barnyakov, A.Yu. @@aut@@ Barnyakov, M.Yu. @@aut@@ Boborovnikov, V.S. @@aut@@ Buzykaev, A.R. @@aut@@ Bykov, A.V. @@aut@@ Danilyuk, A.F. @@aut@@ Katcin, A.A. @@aut@@ Kononov, S.A. @@aut@@ Korda, D.V. @@aut@@ Kravchenko, E.A. @@aut@@ Kuyanov, I.A. @@aut@@ Onuchin, A.P. @@aut@@ Ovtin, I.V. @@aut@@ Podgornov, N.A. @@aut@@ Porosev, V.V. @@aut@@ Razuvaev, G.P. @@aut@@ Rodiakin, V.A. @@aut@@ Todyshev, K.Yu. @@aut@@ Vorobyev, V.S. @@aut@@ |
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530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Particle identification system for the Super Charm–Tau Factory at Novosibirsk Aerogel RICH ToF TOP Shifter ASHIPH PID system Particle separation |
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Barnyakov, A.Yu. Barnyakov, M.Yu. Boborovnikov, V.S. Buzykaev, A.R. Bykov, A.V. Danilyuk, A.F. Katcin, A.A. Kononov, S.A. Korda, D.V. Kravchenko, E.A. Kuyanov, I.A. Onuchin, A.P. Ovtin, I.V. Podgornov, N.A. Porosev, V.V. Razuvaev, G.P. Rodiakin, V.A. Todyshev, K.Yu. Vorobyev, V.S. |
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particle identification system for the super charm–tau factory at novosibirsk |
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Particle identification system for the Super Charm–Tau Factory at Novosibirsk |
| abstract |
The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. |
| abstractGer |
The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. |
| abstract_unstemmed |
The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. The interaction region should be equipped by an excellent universal particle detector meeting the requirements of broad physics program of the experiment. Research and development for all detector subsystems is currently underway. Particle identification (PID) system of the detector is required to provide the state-of-the-art level of μ / π separation for the particle momenta up to 1 . 2 GeV∕c . The following options for the PID system are considered in this paper: focusing aerogel ring imaging Cherenkov (FARICH) detector composed of 4-layer aerogel tiles, threshold Cherenkov counters based on aerogel shifter photomultiplier (ASHIPH), and time-of-flight (ToF) detector combined with the time-of-propagation (ToP) approach providing a time resolution better than 30 ps . Assessment of the charged particle separation performance for these options based on simulation and prototype tests results is presented. |
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Particle identification system for the Super Charm–Tau Factory at Novosibirsk |
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Barnyakov, M.Yu Boborovnikov, V.S. Buzykaev, A.R. Bykov, A.V. Danilyuk, A.F. Katcin, A.A. Kononov, S.A. Korda, D.V. Kravchenko, E.A. Kuyanov, I.A. Onuchin, A.P. Ovtin, I.V. Podgornov, N.A. Porosev, V.V. Razuvaev, G.P. Rodiakin, V.A. Todyshev, K.Yu Vorobyev, V.S. |
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Barnyakov, M.Yu Boborovnikov, V.S. Buzykaev, A.R. Bykov, A.V. Danilyuk, A.F. Katcin, A.A. Kononov, S.A. Korda, D.V. Kravchenko, E.A. Kuyanov, I.A. Onuchin, A.P. Ovtin, I.V. Podgornov, N.A. Porosev, V.V. Razuvaev, G.P. Rodiakin, V.A. Todyshev, K.Yu Vorobyev, V.S. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV003681157</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230524125849.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230501s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.nima.2019.162352</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV003681157</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0168-9002(19)30932-5</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rda</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.05</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.07</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.40</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Barnyakov, A.Yu.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Particle identification system for the Super Charm–Tau Factory at Novosibirsk</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</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="520" ind1=" " ind2=" "><subfield code="a">The Super Charm–Tau (SCT) Factory is a proposed electron–positron collider in Novosibirsk with a peak luminosity of 1 0 35 cm − 1 s − 1 operating in the energy range between 2and 6 GeV. 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