Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction
A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation dete...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Masuda, A [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
lithium-6-glass scintillation detector quasi-monoenergetic high-energy neutron field organic liquid scintillation detector |
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| Übergeordnetes Werk: |
Enthalten in: IEEE transactions on nuclear science - New York, NY : IEEE, 1963, 62(2015), 3, Seite 1295-1300 |
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| Übergeordnetes Werk: |
volume:62 ; year:2015 ; number:3 ; pages:1295-1300 |
| Links: |
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| DOI / URN: |
10.1109/TNS.2015.2432273 |
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| Katalog-ID: |
OLC1966224184 |
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| 264 | 1 | |c 2015 | |
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| 520 | |a A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. | ||
| 650 | 4 | |a lithium-6-glass scintillation detector | |
| 650 | 4 | |a time of flight spectroscopy | |
| 650 | 4 | |a spectrometry | |
| 650 | 4 | |a neutron detectors | |
| 650 | 4 | |a beam chopping system | |
| 650 | 4 | |a quasi-monoenergetic high-energy neutron field | |
| 650 | 4 | |a time-of-flight measurements | |
| 650 | 4 | |a organic liquid scintillation detector | |
| 650 | 4 | |a Collimators | |
| 650 | 4 | |a proton-nucleus reactions | |
| 650 | 4 | |a time-of-flight method | |
| 650 | 4 | |a Detectors | |
| 650 | 4 | |a Particle beams | |
| 650 | 4 | |a room-scattered neutrons | |
| 650 | 4 | |a 7 Li(proton | |
| 650 | 4 | |a quasi-monoenergetic neutron fields | |
| 650 | 4 | |a Neutrons | |
| 650 | 4 | |a High-energy neutrons | |
| 650 | 4 | |a neutron spectral fluence | |
| 650 | 4 | |a Cyclotrons | |
| 650 | 4 | |a neutron | |
| 650 | 4 | |a Liquids | |
| 650 | 4 | |a neutron detection | |
| 650 | 4 | |a time-independent neutrons | |
| 650 | 4 | |a Energy measurement | |
| 700 | 1 | |a Matsumoto, T |4 oth | |
| 700 | 1 | |a Harano, H |4 oth | |
| 700 | 1 | |a Tanimura, Y |4 oth | |
| 700 | 1 | |a Shikaze, Y |4 oth | |
| 700 | 1 | |a Yoshitomi, H |4 oth | |
| 700 | 1 | |a Nishino, S |4 oth | |
| 700 | 1 | |a Kurashima, S |4 oth | |
| 700 | 1 | |a Hagiwara, M |4 oth | |
| 700 | 1 | |a Unno, Y |4 oth | |
| 700 | 1 | |a Nishiyama, J |4 oth | |
| 700 | 1 | |a Yoshizawa, M |4 oth | |
| 700 | 1 | |a Seito, H |4 oth | |
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10.1109/TNS.2015.2432273 doi PQ20160617 (DE-627)OLC1966224184 (DE-599)GBVOLC1966224184 (PRQ)c701-bca44aa852563ebe2a968604270fd8701badb989dc5dbad99a8bd2f2e238279b0 (KEY)0054996720150000062000301295timeofflightmeasurementsforlowenergycomponentsof45 DE-627 ger DE-627 rakwb eng 620 DNB Masuda, A verfasserin aut Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. lithium-6-glass scintillation detector time of flight spectroscopy spectrometry neutron detectors beam chopping system quasi-monoenergetic high-energy neutron field time-of-flight measurements organic liquid scintillation detector Collimators proton-nucleus reactions time-of-flight method Detectors Particle beams room-scattered neutrons 7 Li(proton quasi-monoenergetic neutron fields Neutrons High-energy neutrons neutron spectral fluence Cyclotrons neutron Liquids neutron detection time-independent neutrons Energy measurement Matsumoto, T oth Harano, H oth Tanimura, Y oth Shikaze, Y oth Yoshitomi, H oth Nishino, S oth Kurashima, S oth Hagiwara, M oth Unno, Y oth Nishiyama, J oth Yoshizawa, M oth Seito, H oth Enthalten in IEEE transactions on nuclear science New York, NY : IEEE, 1963 62(2015), 3, Seite 1295-1300 (DE-627)129547352 (DE-600)218510-6 (DE-576)014998238 0018-9499 nnns volume:62 year:2015 number:3 pages:1295-1300 http://dx.doi.org/10.1109/TNS.2015.2432273 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7117468 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-PHA GBV_ILN_70 AR 62 2015 3 1295-1300 |
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10.1109/TNS.2015.2432273 doi PQ20160617 (DE-627)OLC1966224184 (DE-599)GBVOLC1966224184 (PRQ)c701-bca44aa852563ebe2a968604270fd8701badb989dc5dbad99a8bd2f2e238279b0 (KEY)0054996720150000062000301295timeofflightmeasurementsforlowenergycomponentsof45 DE-627 ger DE-627 rakwb eng 620 DNB Masuda, A verfasserin aut Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. lithium-6-glass scintillation detector time of flight spectroscopy spectrometry neutron detectors beam chopping system quasi-monoenergetic high-energy neutron field time-of-flight measurements organic liquid scintillation detector Collimators proton-nucleus reactions time-of-flight method Detectors Particle beams room-scattered neutrons 7 Li(proton quasi-monoenergetic neutron fields Neutrons High-energy neutrons neutron spectral fluence Cyclotrons neutron Liquids neutron detection time-independent neutrons Energy measurement Matsumoto, T oth Harano, H oth Tanimura, Y oth Shikaze, Y oth Yoshitomi, H oth Nishino, S oth Kurashima, S oth Hagiwara, M oth Unno, Y oth Nishiyama, J oth Yoshizawa, M oth Seito, H oth Enthalten in IEEE transactions on nuclear science New York, NY : IEEE, 1963 62(2015), 3, Seite 1295-1300 (DE-627)129547352 (DE-600)218510-6 (DE-576)014998238 0018-9499 nnns volume:62 year:2015 number:3 pages:1295-1300 http://dx.doi.org/10.1109/TNS.2015.2432273 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7117468 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-PHA GBV_ILN_70 AR 62 2015 3 1295-1300 |
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10.1109/TNS.2015.2432273 doi PQ20160617 (DE-627)OLC1966224184 (DE-599)GBVOLC1966224184 (PRQ)c701-bca44aa852563ebe2a968604270fd8701badb989dc5dbad99a8bd2f2e238279b0 (KEY)0054996720150000062000301295timeofflightmeasurementsforlowenergycomponentsof45 DE-627 ger DE-627 rakwb eng 620 DNB Masuda, A verfasserin aut Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. lithium-6-glass scintillation detector time of flight spectroscopy spectrometry neutron detectors beam chopping system quasi-monoenergetic high-energy neutron field time-of-flight measurements organic liquid scintillation detector Collimators proton-nucleus reactions time-of-flight method Detectors Particle beams room-scattered neutrons 7 Li(proton quasi-monoenergetic neutron fields Neutrons High-energy neutrons neutron spectral fluence Cyclotrons neutron Liquids neutron detection time-independent neutrons Energy measurement Matsumoto, T oth Harano, H oth Tanimura, Y oth Shikaze, Y oth Yoshitomi, H oth Nishino, S oth Kurashima, S oth Hagiwara, M oth Unno, Y oth Nishiyama, J oth Yoshizawa, M oth Seito, H oth Enthalten in IEEE transactions on nuclear science New York, NY : IEEE, 1963 62(2015), 3, Seite 1295-1300 (DE-627)129547352 (DE-600)218510-6 (DE-576)014998238 0018-9499 nnns volume:62 year:2015 number:3 pages:1295-1300 http://dx.doi.org/10.1109/TNS.2015.2432273 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7117468 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-PHA GBV_ILN_70 AR 62 2015 3 1295-1300 |
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10.1109/TNS.2015.2432273 doi PQ20160617 (DE-627)OLC1966224184 (DE-599)GBVOLC1966224184 (PRQ)c701-bca44aa852563ebe2a968604270fd8701badb989dc5dbad99a8bd2f2e238279b0 (KEY)0054996720150000062000301295timeofflightmeasurementsforlowenergycomponentsof45 DE-627 ger DE-627 rakwb eng 620 DNB Masuda, A verfasserin aut Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. lithium-6-glass scintillation detector time of flight spectroscopy spectrometry neutron detectors beam chopping system quasi-monoenergetic high-energy neutron field time-of-flight measurements organic liquid scintillation detector Collimators proton-nucleus reactions time-of-flight method Detectors Particle beams room-scattered neutrons 7 Li(proton quasi-monoenergetic neutron fields Neutrons High-energy neutrons neutron spectral fluence Cyclotrons neutron Liquids neutron detection time-independent neutrons Energy measurement Matsumoto, T oth Harano, H oth Tanimura, Y oth Shikaze, Y oth Yoshitomi, H oth Nishino, S oth Kurashima, S oth Hagiwara, M oth Unno, Y oth Nishiyama, J oth Yoshizawa, M oth Seito, H oth Enthalten in IEEE transactions on nuclear science New York, NY : IEEE, 1963 62(2015), 3, Seite 1295-1300 (DE-627)129547352 (DE-600)218510-6 (DE-576)014998238 0018-9499 nnns volume:62 year:2015 number:3 pages:1295-1300 http://dx.doi.org/10.1109/TNS.2015.2432273 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7117468 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-PHA GBV_ILN_70 AR 62 2015 3 1295-1300 |
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10.1109/TNS.2015.2432273 doi PQ20160617 (DE-627)OLC1966224184 (DE-599)GBVOLC1966224184 (PRQ)c701-bca44aa852563ebe2a968604270fd8701badb989dc5dbad99a8bd2f2e238279b0 (KEY)0054996720150000062000301295timeofflightmeasurementsforlowenergycomponentsof45 DE-627 ger DE-627 rakwb eng 620 DNB Masuda, A verfasserin aut Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. lithium-6-glass scintillation detector time of flight spectroscopy spectrometry neutron detectors beam chopping system quasi-monoenergetic high-energy neutron field time-of-flight measurements organic liquid scintillation detector Collimators proton-nucleus reactions time-of-flight method Detectors Particle beams room-scattered neutrons 7 Li(proton quasi-monoenergetic neutron fields Neutrons High-energy neutrons neutron spectral fluence Cyclotrons neutron Liquids neutron detection time-independent neutrons Energy measurement Matsumoto, T oth Harano, H oth Tanimura, Y oth Shikaze, Y oth Yoshitomi, H oth Nishino, S oth Kurashima, S oth Hagiwara, M oth Unno, Y oth Nishiyama, J oth Yoshizawa, M oth Seito, H oth Enthalten in IEEE transactions on nuclear science New York, NY : IEEE, 1963 62(2015), 3, Seite 1295-1300 (DE-627)129547352 (DE-600)218510-6 (DE-576)014998238 0018-9499 nnns volume:62 year:2015 number:3 pages:1295-1300 http://dx.doi.org/10.1109/TNS.2015.2432273 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7117468 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-PHA GBV_ILN_70 AR 62 2015 3 1295-1300 |
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Masuda, A @@aut@@ Matsumoto, T @@oth@@ Harano, H @@oth@@ Tanimura, Y @@oth@@ Shikaze, Y @@oth@@ Yoshitomi, H @@oth@@ Nishino, S @@oth@@ Kurashima, S @@oth@@ Hagiwara, M @@oth@@ Unno, Y @@oth@@ Nishiyama, J @@oth@@ Yoshizawa, M @@oth@@ Seito, H @@oth@@ |
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Masuda, A ddc 620 misc lithium-6-glass scintillation detector misc time of flight spectroscopy misc spectrometry misc neutron detectors misc beam chopping system misc quasi-monoenergetic high-energy neutron field misc time-of-flight measurements misc organic liquid scintillation detector misc Collimators misc proton-nucleus reactions misc time-of-flight method misc Detectors misc Particle beams misc room-scattered neutrons misc 7 Li(proton misc quasi-monoenergetic neutron fields misc Neutrons misc High-energy neutrons misc neutron spectral fluence misc Cyclotrons misc neutron misc Liquids misc neutron detection misc time-independent neutrons misc Energy measurement Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction |
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620 DNB Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction lithium-6-glass scintillation detector time of flight spectroscopy spectrometry neutron detectors beam chopping system quasi-monoenergetic high-energy neutron field time-of-flight measurements organic liquid scintillation detector Collimators proton-nucleus reactions time-of-flight method Detectors Particle beams room-scattered neutrons 7 Li(proton quasi-monoenergetic neutron fields Neutrons High-energy neutrons neutron spectral fluence Cyclotrons neutron Liquids neutron detection time-independent neutrons Energy measurement |
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ddc 620 misc lithium-6-glass scintillation detector misc time of flight spectroscopy misc spectrometry misc neutron detectors misc beam chopping system misc quasi-monoenergetic high-energy neutron field misc time-of-flight measurements misc organic liquid scintillation detector misc Collimators misc proton-nucleus reactions misc time-of-flight method misc Detectors misc Particle beams misc room-scattered neutrons misc 7 Li(proton misc quasi-monoenergetic neutron fields misc Neutrons misc High-energy neutrons misc neutron spectral fluence misc Cyclotrons misc neutron misc Liquids misc neutron detection misc time-independent neutrons misc Energy measurement |
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Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction |
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Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction |
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time-of-flight measurements for low-energy components of 45-mev quasi-monoenergetic high-energy neutron field from (, )} reaction |
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Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction |
| abstract |
A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. |
| abstractGer |
A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. |
| abstract_unstemmed |
A quasi-monoenergetic neutron field generated in the 7 Li(p, n) reaction consists of a high-energy monoenergetic peak and a continuum to the low-energy region. In this study, the spectral fluence of the continuum was measured with the time-of-flight (TOF) method using a 6 Li-glass scintillation detector and an organic liquid scintillation detector for the keV and MeV region, respectively. The neutron spectral fluence was determined down to the keV region by implementing a new beam chopping system and the results showed that the neutrons that came directly from the target had a lower energy limit about 100 keV. Discussions were made also on the effect of the time-independent neutrons which are assumed to be room-scattered neutrons. The obtained information is expected to contribute to understanding the quasi-monoenergetic high-energy neutron field and improvements of calibrating neutron detectors in the field. |
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Time-of-Flight Measurements for Low-Energy Components of 45-MeV Quasi-Monoenergetic High-Energy Neutron Field from (, )} Reaction |
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Matsumoto, T Harano, H Tanimura, Y Shikaze, Y Yoshitomi, H Nishino, S Kurashima, S Hagiwara, M Unno, Y Nishiyama, J Yoshizawa, M Seito, H |
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Matsumoto, T Harano, H Tanimura, Y Shikaze, Y Yoshitomi, H Nishino, S Kurashima, S Hagiwara, M Unno, Y Nishiyama, J Yoshizawa, M Seito, H |
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