A new large-acceptance and high-efficiency neutron detector for missing-mass studies
Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. Th...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bollini, D. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1969 |
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| Schlagwörter: |
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| Anmerkung: |
© Società Italiana di Fisica 1969 |
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| Übergeordnetes Werk: |
Enthalten in: Il nuovo cimento - [S.l.] : Italian Physical Society, 1965, 61(1969), 2 vom: Mai, Seite 125-172 |
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| Übergeordnetes Werk: |
volume:61 ; year:1969 ; number:2 ; month:05 ; pages:125-172 |
| Links: |
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| DOI / URN: |
10.1007/BF02755121 |
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| Katalog-ID: |
SPR020629680 |
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|---|---|---|---|
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| 008 | 201006s1969 xx |||||o 00| ||eng c | ||
| 024 | 7 | |a 10.1007/BF02755121 |2 doi | |
| 035 | |a (DE-627)SPR020629680 | ||
| 035 | |a (SPR)BF02755121-e | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 100 | 1 | |a Bollini, D. |e verfasserin |4 aut | |
| 245 | 1 | 2 | |a A new large-acceptance and high-efficiency neutron detector for missing-mass studies |
| 264 | 1 | |c 1969 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
| 338 | |a Online-Ressource |b cr |2 rdacarrier | ||
| 500 | |a © Società Italiana di Fisica 1969 | ||
| 520 | |a Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. | ||
| 650 | 4 | |a Neutron Detector |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Plastic Scintillator |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neutron Counter |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Attenuation Length |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neutron Time |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Buhler-Broglin, A. |4 aut | |
| 700 | 1 | |a Dalpiaz, P. |4 aut | |
| 700 | 1 | |a Massam, T. |4 aut | |
| 700 | 1 | |a Navach, F. |4 aut | |
| 700 | 1 | |a Navarria, F. L. |4 aut | |
| 700 | 1 | |a Schneegans, M. A. |4 aut | |
| 700 | 1 | |a Zetti, F. |4 aut | |
| 700 | 1 | |a Zichichi, A. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Il nuovo cimento |d [S.l.] : Italian Physical Society, 1965 |g 61(1969), 2 vom: Mai, Seite 125-172 |w (DE-627)627248667 |w (DE-600)2556213-7 |x 1826-9869 |7 nnns |
| 773 | 1 | 8 | |g volume:61 |g year:1969 |g number:2 |g month:05 |g pages:125-172 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/BF02755121 |z lizenzpflichtig |3 Volltext |
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| 912 | |a GBV_ILN_2034 | ||
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| 912 | |a GBV_ILN_2055 | ||
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| 912 | |a GBV_ILN_2059 | ||
| 912 | |a GBV_ILN_2061 | ||
| 912 | |a GBV_ILN_2064 | ||
| 912 | |a GBV_ILN_2065 | ||
| 912 | |a GBV_ILN_2068 | ||
| 912 | |a GBV_ILN_2088 | ||
| 912 | |a GBV_ILN_2093 | ||
| 912 | |a GBV_ILN_2106 | ||
| 912 | |a GBV_ILN_2107 | ||
| 912 | |a GBV_ILN_2108 | ||
| 912 | |a GBV_ILN_2110 | ||
| 912 | |a GBV_ILN_2111 | ||
| 912 | |a GBV_ILN_2112 | ||
| 912 | |a GBV_ILN_2113 | ||
| 912 | |a GBV_ILN_2116 | ||
| 912 | |a GBV_ILN_2118 | ||
| 912 | |a GBV_ILN_2119 | ||
| 912 | |a GBV_ILN_2122 | ||
| 912 | |a GBV_ILN_2129 | ||
| 912 | |a GBV_ILN_2143 | ||
| 912 | |a GBV_ILN_2144 | ||
| 912 | |a GBV_ILN_2147 | ||
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| 912 | |a GBV_ILN_2152 | ||
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| 912 | |a GBV_ILN_2193 | ||
| 912 | |a GBV_ILN_2232 | ||
| 912 | |a GBV_ILN_2336 | ||
| 912 | |a GBV_ILN_2446 | ||
| 912 | |a GBV_ILN_2470 | ||
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| 912 | |a GBV_ILN_4112 | ||
| 912 | |a GBV_ILN_4125 | ||
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| 912 | |a GBV_ILN_4242 | ||
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| 912 | |a GBV_ILN_4251 | ||
| 912 | |a GBV_ILN_4277 | ||
| 912 | |a GBV_ILN_4305 | ||
| 912 | |a GBV_ILN_4306 | ||
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| 912 | |a GBV_ILN_4313 | ||
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| 912 | |a GBV_ILN_4325 | ||
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| 951 | |a AR | ||
| 952 | |d 61 |j 1969 |e 2 |c 05 |h 125-172 | ||
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1969 |
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1969 |
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10.1007/BF02755121 doi (DE-627)SPR020629680 (SPR)BF02755121-e DE-627 ger DE-627 rakwb eng Bollini, D. verfasserin aut A new large-acceptance and high-efficiency neutron detector for missing-mass studies 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. Neutron Detector (dpeaa)DE-He213 Plastic Scintillator (dpeaa)DE-He213 Neutron Counter (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Neutron Time (dpeaa)DE-He213 Buhler-Broglin, A. aut Dalpiaz, P. aut Massam, T. aut Navach, F. aut Navarria, F. L. aut Schneegans, M. A. aut Zetti, F. aut Zichichi, A. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 61(1969), 2 vom: Mai, Seite 125-172 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:61 year:1969 number:2 month:05 pages:125-172 https://dx.doi.org/10.1007/BF02755121 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 61 1969 2 05 125-172 |
| spelling |
10.1007/BF02755121 doi (DE-627)SPR020629680 (SPR)BF02755121-e DE-627 ger DE-627 rakwb eng Bollini, D. verfasserin aut A new large-acceptance and high-efficiency neutron detector for missing-mass studies 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. Neutron Detector (dpeaa)DE-He213 Plastic Scintillator (dpeaa)DE-He213 Neutron Counter (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Neutron Time (dpeaa)DE-He213 Buhler-Broglin, A. aut Dalpiaz, P. aut Massam, T. aut Navach, F. aut Navarria, F. L. aut Schneegans, M. A. aut Zetti, F. aut Zichichi, A. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 61(1969), 2 vom: Mai, Seite 125-172 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:61 year:1969 number:2 month:05 pages:125-172 https://dx.doi.org/10.1007/BF02755121 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 61 1969 2 05 125-172 |
| allfields_unstemmed |
10.1007/BF02755121 doi (DE-627)SPR020629680 (SPR)BF02755121-e DE-627 ger DE-627 rakwb eng Bollini, D. verfasserin aut A new large-acceptance and high-efficiency neutron detector for missing-mass studies 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. Neutron Detector (dpeaa)DE-He213 Plastic Scintillator (dpeaa)DE-He213 Neutron Counter (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Neutron Time (dpeaa)DE-He213 Buhler-Broglin, A. aut Dalpiaz, P. aut Massam, T. aut Navach, F. aut Navarria, F. L. aut Schneegans, M. A. aut Zetti, F. aut Zichichi, A. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 61(1969), 2 vom: Mai, Seite 125-172 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:61 year:1969 number:2 month:05 pages:125-172 https://dx.doi.org/10.1007/BF02755121 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 61 1969 2 05 125-172 |
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10.1007/BF02755121 doi (DE-627)SPR020629680 (SPR)BF02755121-e DE-627 ger DE-627 rakwb eng Bollini, D. verfasserin aut A new large-acceptance and high-efficiency neutron detector for missing-mass studies 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. Neutron Detector (dpeaa)DE-He213 Plastic Scintillator (dpeaa)DE-He213 Neutron Counter (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Neutron Time (dpeaa)DE-He213 Buhler-Broglin, A. aut Dalpiaz, P. aut Massam, T. aut Navach, F. aut Navarria, F. L. aut Schneegans, M. A. aut Zetti, F. aut Zichichi, A. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 61(1969), 2 vom: Mai, Seite 125-172 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:61 year:1969 number:2 month:05 pages:125-172 https://dx.doi.org/10.1007/BF02755121 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 61 1969 2 05 125-172 |
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10.1007/BF02755121 doi (DE-627)SPR020629680 (SPR)BF02755121-e DE-627 ger DE-627 rakwb eng Bollini, D. verfasserin aut A new large-acceptance and high-efficiency neutron detector for missing-mass studies 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. Neutron Detector (dpeaa)DE-He213 Plastic Scintillator (dpeaa)DE-He213 Neutron Counter (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Neutron Time (dpeaa)DE-He213 Buhler-Broglin, A. aut Dalpiaz, P. aut Massam, T. aut Navach, F. aut Navarria, F. L. aut Schneegans, M. A. aut Zetti, F. aut Zichichi, A. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Society, 1965 61(1969), 2 vom: Mai, Seite 125-172 (DE-627)627248667 (DE-600)2556213-7 1826-9869 nnns volume:61 year:1969 number:2 month:05 pages:125-172 https://dx.doi.org/10.1007/BF02755121 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 61 1969 2 05 125-172 |
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English |
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Enthalten in Il nuovo cimento 61(1969), 2 vom: Mai, Seite 125-172 volume:61 year:1969 number:2 month:05 pages:125-172 |
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Enthalten in Il nuovo cimento 61(1969), 2 vom: Mai, Seite 125-172 volume:61 year:1969 number:2 month:05 pages:125-172 |
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Neutron Detector Plastic Scintillator Neutron Counter Attenuation Length Neutron Time |
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Il nuovo cimento |
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Bollini, D. @@aut@@ Buhler-Broglin, A. @@aut@@ Dalpiaz, P. @@aut@@ Massam, T. @@aut@@ Navach, F. @@aut@@ Navarria, F. L. @@aut@@ Schneegans, M. A. @@aut@@ Zetti, F. @@aut@@ Zichichi, A. @@aut@@ |
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1969-05-01T00:00:00Z |
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The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. 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Bollini, D. |
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A new large-acceptance and high-efficiency neutron detector for missing-mass studies Neutron Detector (dpeaa)DE-He213 Plastic Scintillator (dpeaa)DE-He213 Neutron Counter (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Neutron Time (dpeaa)DE-He213 |
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Elektronische Aufsätze |
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Bollini, D. |
| doi_str_mv |
10.1007/BF02755121 |
| title_sort |
new large-acceptance and high-efficiency neutron detector for missing-mass studies |
| title_auth |
A new large-acceptance and high-efficiency neutron detector for missing-mass studies |
| abstract |
Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. © Società Italiana di Fisica 1969 |
| abstractGer |
Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. © Società Italiana di Fisica 1969 |
| abstract_unstemmed |
Summary A large-acceptance and high-efficiency neutron detector is described. The sensitive surface and volume of the detector are 2.16 $ m^{2} $ and 0.78 $ m^{3} $, respectively. The detector consists of twenty-four elements of plastic scintillator, each having dimensions (100×18×18) $ cm^{3} $. The large volume of scintillator, in the particular geometrical arrangement chosen, allows a mean detection efficiency of about 25% in the range (70÷390) MeV neutron kinetic energy for a laboratory solid angle of 0.14 sr at 4 m radial distance. With the techniques adopted, calibrations with charged particles can be easily performed in a few hours using a low beam intensity. An interesting features of this instrument is the accuracy achieved in locating incident particles, which is ±1.4 cm for charged particles, and ±2.5 cm for neutrons. The accuracies achieved for the time-of-flight measurement are ±0.35 ns for charged particles and ±0.7 ns for neutrons. With these resolutions in the neutron time of flight and angle, the uncertainty in the missing mass is ±4 MeV for η, ±10 MeV for ω, and ±15 MeV for ϕ mesons. © Società Italiana di Fisica 1969 |
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| title_short |
A new large-acceptance and high-efficiency neutron detector for missing-mass studies |
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https://dx.doi.org/10.1007/BF02755121 |
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Buhler-Broglin, A. Dalpiaz, P. Massam, T. Navach, F. Navarria, F. L. Schneegans, M. A. Zetti, F. Zichichi, A. |
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Buhler-Broglin, A. Dalpiaz, P. Massam, T. Navach, F. Navarria, F. L. Schneegans, M. A. Zetti, F. Zichichi, A. |
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| score |
7.3987446 |