Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion
Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contra...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kadykov, M. G. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013 |
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| Schlagwörter: |
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| Anmerkung: |
© Pleiades Publishing, Ltd. 2013 |
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| Übergeordnetes Werk: |
Enthalten in: Physics of particles and nuclei letters - Berlin : Springer, 2006, 10(2013), 6 vom: Nov., Seite 573-579 |
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| Übergeordnetes Werk: |
volume:10 ; year:2013 ; number:6 ; month:11 ; pages:573-579 |
| Links: |
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| DOI / URN: |
10.1134/S1547477113060137 |
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| Katalog-ID: |
SPR020224117 |
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| 100 | 1 | |a Kadykov, M. G. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion |
| 264 | 1 | |c 2013 | |
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| 520 | |a Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. | ||
| 650 | 4 | |a Nucleus Letter |7 (dpeaa)DE-He213 | |
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| 650 | 4 | |a Reference Spectrum |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neutron Spectrum |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Effective Cross Section |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Korneev, S. V. |4 aut | |
| 700 | 1 | |a Martsynkevich, B. A. |4 aut | |
| 700 | 1 | |a Tyutyunnikov, S. I. |4 aut | |
| 700 | 1 | |a Khil’manovich, A. M. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Physics of particles and nuclei letters |d Berlin : Springer, 2006 |g 10(2013), 6 vom: Nov., Seite 573-579 |w (DE-627)509758479 |w (DE-600)2228439-4 |x 1531-8567 |7 nnns |
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10.1134/S1547477113060137 doi (DE-627)SPR020224117 (SPR)S1547477113060137-e DE-627 ger DE-627 rakwb eng Kadykov, M. G. verfasserin aut Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. Nucleus Letter (dpeaa)DE-He213 Reaction Cross Section (dpeaa)DE-He213 Reference Spectrum (dpeaa)DE-He213 Neutron Spectrum (dpeaa)DE-He213 Effective Cross Section (dpeaa)DE-He213 Korneev, S. V. aut Martsynkevich, B. A. aut Tyutyunnikov, S. I. aut Khil’manovich, A. M. aut Enthalten in Physics of particles and nuclei letters Berlin : Springer, 2006 10(2013), 6 vom: Nov., Seite 573-579 (DE-627)509758479 (DE-600)2228439-4 1531-8567 nnns volume:10 year:2013 number:6 month:11 pages:573-579 https://dx.doi.org/10.1134/S1547477113060137 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 AR 10 2013 6 11 573-579 |
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10.1134/S1547477113060137 doi (DE-627)SPR020224117 (SPR)S1547477113060137-e DE-627 ger DE-627 rakwb eng Kadykov, M. G. verfasserin aut Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. Nucleus Letter (dpeaa)DE-He213 Reaction Cross Section (dpeaa)DE-He213 Reference Spectrum (dpeaa)DE-He213 Neutron Spectrum (dpeaa)DE-He213 Effective Cross Section (dpeaa)DE-He213 Korneev, S. V. aut Martsynkevich, B. A. aut Tyutyunnikov, S. I. aut Khil’manovich, A. M. aut Enthalten in Physics of particles and nuclei letters Berlin : Springer, 2006 10(2013), 6 vom: Nov., Seite 573-579 (DE-627)509758479 (DE-600)2228439-4 1531-8567 nnns volume:10 year:2013 number:6 month:11 pages:573-579 https://dx.doi.org/10.1134/S1547477113060137 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 AR 10 2013 6 11 573-579 |
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10.1134/S1547477113060137 doi (DE-627)SPR020224117 (SPR)S1547477113060137-e DE-627 ger DE-627 rakwb eng Kadykov, M. G. verfasserin aut Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. Nucleus Letter (dpeaa)DE-He213 Reaction Cross Section (dpeaa)DE-He213 Reference Spectrum (dpeaa)DE-He213 Neutron Spectrum (dpeaa)DE-He213 Effective Cross Section (dpeaa)DE-He213 Korneev, S. V. aut Martsynkevich, B. A. aut Tyutyunnikov, S. I. aut Khil’manovich, A. M. aut Enthalten in Physics of particles and nuclei letters Berlin : Springer, 2006 10(2013), 6 vom: Nov., Seite 573-579 (DE-627)509758479 (DE-600)2228439-4 1531-8567 nnns volume:10 year:2013 number:6 month:11 pages:573-579 https://dx.doi.org/10.1134/S1547477113060137 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 AR 10 2013 6 11 573-579 |
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10.1134/S1547477113060137 doi (DE-627)SPR020224117 (SPR)S1547477113060137-e DE-627 ger DE-627 rakwb eng Kadykov, M. G. verfasserin aut Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. Nucleus Letter (dpeaa)DE-He213 Reaction Cross Section (dpeaa)DE-He213 Reference Spectrum (dpeaa)DE-He213 Neutron Spectrum (dpeaa)DE-He213 Effective Cross Section (dpeaa)DE-He213 Korneev, S. V. aut Martsynkevich, B. A. aut Tyutyunnikov, S. I. aut Khil’manovich, A. M. aut Enthalten in Physics of particles and nuclei letters Berlin : Springer, 2006 10(2013), 6 vom: Nov., Seite 573-579 (DE-627)509758479 (DE-600)2228439-4 1531-8567 nnns volume:10 year:2013 number:6 month:11 pages:573-579 https://dx.doi.org/10.1134/S1547477113060137 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 AR 10 2013 6 11 573-579 |
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10.1134/S1547477113060137 doi (DE-627)SPR020224117 (SPR)S1547477113060137-e DE-627 ger DE-627 rakwb eng Kadykov, M. G. verfasserin aut Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. Nucleus Letter (dpeaa)DE-He213 Reaction Cross Section (dpeaa)DE-He213 Reference Spectrum (dpeaa)DE-He213 Neutron Spectrum (dpeaa)DE-He213 Effective Cross Section (dpeaa)DE-He213 Korneev, S. V. aut Martsynkevich, B. A. aut Tyutyunnikov, S. I. aut Khil’manovich, A. M. aut Enthalten in Physics of particles and nuclei letters Berlin : Springer, 2006 10(2013), 6 vom: Nov., Seite 573-579 (DE-627)509758479 (DE-600)2228439-4 1531-8567 nnns volume:10 year:2013 number:6 month:11 pages:573-579 https://dx.doi.org/10.1134/S1547477113060137 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 AR 10 2013 6 11 573-579 |
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Enthalten in Physics of particles and nuclei letters 10(2013), 6 vom: Nov., Seite 573-579 volume:10 year:2013 number:6 month:11 pages:573-579 |
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Kadykov, M. G. @@aut@@ Korneev, S. V. @@aut@@ Martsynkevich, B. A. @@aut@@ Tyutyunnikov, S. I. @@aut@@ Khil’manovich, A. M. @@aut@@ |
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Kadykov, M. G. |
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Kadykov, M. G. misc Nucleus Letter misc Reaction Cross Section misc Reference Spectrum misc Neutron Spectrum misc Effective Cross Section Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion |
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Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion Nucleus Letter (dpeaa)DE-He213 Reaction Cross Section (dpeaa)DE-He213 Reference Spectrum (dpeaa)DE-He213 Neutron Spectrum (dpeaa)DE-He213 Effective Cross Section (dpeaa)DE-He213 |
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Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion |
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Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion |
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reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a legendre polynomial expansion |
| title_auth |
Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion |
| abstract |
Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. © Pleiades Publishing, Ltd. 2013 |
| abstractGer |
Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. © Pleiades Publishing, Ltd. 2013 |
| abstract_unstemmed |
Abstract This paper proposes a method for reconstructing the fast neutron spectra in the range 0.2 MeV to 100 MeV based on modified methods of the effective threshold cross sections and the deformation of a reference spectrum using the Legendre polynomial expansion of a deforming function. In contrast to the deformation method traditionally used to determine the desired differential spectrum φ(E), we propose the use of a deforming function as a Legendre polynomial expansion in order to determine the integrated spectrum F(E). Since F(E) is a monotonic decreasing function that tends to zero when approaching the maximum spectral energy, it can be represented by a shorter series; i.e., the number M of the sought series coefficients am will not be large. The developed program was used to calculate fast neutron spectra in a QUINTA nuclear setup that was irradiated with 1–8 GeV deuterons of Nuclotron-M at the Laboratory of High Energies of the Joint Institute for Nuclear Research. © Pleiades Publishing, Ltd. 2013 |
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Reconstruction of the fast neutron spectrum using deformation of a reference spectrum represented as a Legendre polynomial expansion |
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https://dx.doi.org/10.1134/S1547477113060137 |
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Korneev, S. V. Martsynkevich, B. A. Tyutyunnikov, S. I. Khil’manovich, A. M. |
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Korneev, S. V. Martsynkevich, B. A. Tyutyunnikov, S. I. Khil’manovich, A. M. |
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10.1134/S1547477113060137 |
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2024-07-03T14:41:16.675Z |
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|
| score |
7.400429 |