Relation of photonuclear reactions to π-meson photoproduction process
Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction unde...
Ausführliche Beschreibung
Autor*in: |
Belousov, A. S. [verfasserIn] Malinovskii, E. I. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2012 |
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Übergeordnetes Werk: |
Enthalten in: Bulletin of the Lebedev Physics Institute - New York, NY : Allerton Press, 1998, 39(2012), 8 vom: Aug., Seite 234-238 |
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Übergeordnetes Werk: |
volume:39 ; year:2012 ; number:8 ; month:08 ; pages:234-238 |
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DOI / URN: |
10.3103/S1068335612080040 |
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Katalog-ID: |
SPR02313898X |
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520 | |a Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. | ||
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700 | 1 | |a Malinovskii, E. I. |e verfasserin |4 aut | |
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10.3103/S1068335612080040 doi (DE-627)SPR02313898X (SPR)S1068335612080040-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Belousov, A. S. verfasserin aut Relation of photonuclear reactions to π-meson photoproduction process 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. spectrometer (dpeaa)DE-He213 gamma activity (dpeaa)DE-He213 photonuclear reactions (dpeaa)DE-He213 photoproduction (dpeaa)DE-He213 isotope (dpeaa)DE-He213 gamma spectrum (dpeaa)DE-He213 isobar (dpeaa)DE-He213 Malinovskii, E. I. verfasserin aut Enthalten in Bulletin of the Lebedev Physics Institute New York, NY : Allerton Press, 1998 39(2012), 8 vom: Aug., Seite 234-238 (DE-627)551157194 (DE-600)2400067-X 1934-838X nnns volume:39 year:2012 number:8 month:08 pages:234-238 https://dx.doi.org/10.3103/S1068335612080040 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2188 GBV_ILN_2190 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 39 2012 8 08 234-238 |
spelling |
10.3103/S1068335612080040 doi (DE-627)SPR02313898X (SPR)S1068335612080040-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Belousov, A. S. verfasserin aut Relation of photonuclear reactions to π-meson photoproduction process 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. spectrometer (dpeaa)DE-He213 gamma activity (dpeaa)DE-He213 photonuclear reactions (dpeaa)DE-He213 photoproduction (dpeaa)DE-He213 isotope (dpeaa)DE-He213 gamma spectrum (dpeaa)DE-He213 isobar (dpeaa)DE-He213 Malinovskii, E. I. verfasserin aut Enthalten in Bulletin of the Lebedev Physics Institute New York, NY : Allerton Press, 1998 39(2012), 8 vom: Aug., Seite 234-238 (DE-627)551157194 (DE-600)2400067-X 1934-838X nnns volume:39 year:2012 number:8 month:08 pages:234-238 https://dx.doi.org/10.3103/S1068335612080040 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2188 GBV_ILN_2190 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 39 2012 8 08 234-238 |
allfields_unstemmed |
10.3103/S1068335612080040 doi (DE-627)SPR02313898X (SPR)S1068335612080040-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Belousov, A. S. verfasserin aut Relation of photonuclear reactions to π-meson photoproduction process 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. spectrometer (dpeaa)DE-He213 gamma activity (dpeaa)DE-He213 photonuclear reactions (dpeaa)DE-He213 photoproduction (dpeaa)DE-He213 isotope (dpeaa)DE-He213 gamma spectrum (dpeaa)DE-He213 isobar (dpeaa)DE-He213 Malinovskii, E. I. verfasserin aut Enthalten in Bulletin of the Lebedev Physics Institute New York, NY : Allerton Press, 1998 39(2012), 8 vom: Aug., Seite 234-238 (DE-627)551157194 (DE-600)2400067-X 1934-838X nnns volume:39 year:2012 number:8 month:08 pages:234-238 https://dx.doi.org/10.3103/S1068335612080040 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2188 GBV_ILN_2190 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 39 2012 8 08 234-238 |
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10.3103/S1068335612080040 doi (DE-627)SPR02313898X (SPR)S1068335612080040-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Belousov, A. S. verfasserin aut Relation of photonuclear reactions to π-meson photoproduction process 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. spectrometer (dpeaa)DE-He213 gamma activity (dpeaa)DE-He213 photonuclear reactions (dpeaa)DE-He213 photoproduction (dpeaa)DE-He213 isotope (dpeaa)DE-He213 gamma spectrum (dpeaa)DE-He213 isobar (dpeaa)DE-He213 Malinovskii, E. I. verfasserin aut Enthalten in Bulletin of the Lebedev Physics Institute New York, NY : Allerton Press, 1998 39(2012), 8 vom: Aug., Seite 234-238 (DE-627)551157194 (DE-600)2400067-X 1934-838X nnns volume:39 year:2012 number:8 month:08 pages:234-238 https://dx.doi.org/10.3103/S1068335612080040 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2188 GBV_ILN_2190 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 39 2012 8 08 234-238 |
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10.3103/S1068335612080040 doi (DE-627)SPR02313898X (SPR)S1068335612080040-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Belousov, A. S. verfasserin aut Relation of photonuclear reactions to π-meson photoproduction process 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. spectrometer (dpeaa)DE-He213 gamma activity (dpeaa)DE-He213 photonuclear reactions (dpeaa)DE-He213 photoproduction (dpeaa)DE-He213 isotope (dpeaa)DE-He213 gamma spectrum (dpeaa)DE-He213 isobar (dpeaa)DE-He213 Malinovskii, E. I. verfasserin aut Enthalten in Bulletin of the Lebedev Physics Institute New York, NY : Allerton Press, 1998 39(2012), 8 vom: Aug., Seite 234-238 (DE-627)551157194 (DE-600)2400067-X 1934-838X nnns volume:39 year:2012 number:8 month:08 pages:234-238 https://dx.doi.org/10.3103/S1068335612080040 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_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 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_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_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2188 GBV_ILN_2190 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 39 2012 8 08 234-238 |
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Belousov, A. S. |
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Belousov, A. S. ddc 530 bkl 33.00 misc spectrometer misc gamma activity misc photonuclear reactions misc photoproduction misc isotope misc gamma spectrum misc isobar Relation of photonuclear reactions to π-meson photoproduction process |
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530 ASE 33.00 bkl Relation of photonuclear reactions to π-meson photoproduction process spectrometer (dpeaa)DE-He213 gamma activity (dpeaa)DE-He213 photonuclear reactions (dpeaa)DE-He213 photoproduction (dpeaa)DE-He213 isotope (dpeaa)DE-He213 gamma spectrum (dpeaa)DE-He213 isobar (dpeaa)DE-He213 |
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ddc 530 bkl 33.00 misc spectrometer misc gamma activity misc photonuclear reactions misc photoproduction misc isotope misc gamma spectrum misc isobar |
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ddc 530 bkl 33.00 misc spectrometer misc gamma activity misc photonuclear reactions misc photoproduction misc isotope misc gamma spectrum misc isobar |
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Relation of photonuclear reactions to π-meson photoproduction process |
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Relation of photonuclear reactions to π-meson photoproduction process |
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Belousov, A. S. Malinovskii, E. I. |
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relation of photonuclear reactions to π-meson photoproduction process |
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Relation of photonuclear reactions to π-meson photoproduction process |
abstract |
Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. |
abstractGer |
Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. |
abstract_unstemmed |
Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $. |
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Relation of photonuclear reactions to π-meson photoproduction process |
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https://dx.doi.org/10.3103/S1068335612080040 |
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S.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Relation of photonuclear reactions to π-meson photoproduction process</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2012</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Neutron-proton pair knocking-out by photons from iron ($ Fe^{56} $) nuclei is studied by measuring induced gamma activity of $ Mn^{54} $ isotope. Experiments are performed in a synchrotron beam at two maximum photon energies, 150 and 650 MeV. It was found that the yield of the reaction under study at the maximum energy of 150 MeV is almost zero, whereas a significant yield of gamma active $ Mn^{54} $ nuclei is measured at the energy of 650 MeV. The cross section of the neutron-proton pair production reaction on $ Fe^{56} $ at an energy of 650 MeV is estimated as 4 · $ 10^{−27} $ $ cm^{2} $.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">spectrometer</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">gamma activity</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">photonuclear reactions</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">photoproduction</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">isotope</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">gamma spectrum</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">isobar</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Malinovskii, E. I.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Bulletin of the Lebedev Physics Institute</subfield><subfield code="d">New York, NY : Allerton Press, 1998</subfield><subfield code="g">39(2012), 8 vom: Aug., Seite 234-238</subfield><subfield code="w">(DE-627)551157194</subfield><subfield code="w">(DE-600)2400067-X</subfield><subfield code="x">1934-838X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:39</subfield><subfield code="g">year:2012</subfield><subfield code="g">number:8</subfield><subfield code="g">month:08</subfield><subfield code="g">pages:234-238</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.3103/S1068335612080040</subfield><subfield code="z">lizenzpflichtig</subfield><subfield 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