Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints
Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficienc...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kuroś-Żołnierczuk, J. [verfasserIn] Thörngren Engblom, P. [verfasserIn] Meyer, H.-O. [verfasserIn] Whitaker, T. J. [verfasserIn] Witała, H. [verfasserIn] Golak, J. [verfasserIn] Kamada, H. [verfasserIn] Nogga, A. [verfasserIn] Skibiński, R. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2004 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Few-body systems - Wien [u.a.] : Springer, 1986, 34(2004), 4 vom: 28. Mai, Seite 259-273 |
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| Übergeordnetes Werk: |
volume:34 ; year:2004 ; number:4 ; day:28 ; month:05 ; pages:259-273 |
| Links: |
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| DOI / URN: |
10.1007/s00601-004-0055-1 |
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| Katalog-ID: |
SPR007044216 |
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| 100 | 1 | |a Kuroś-Żołnierczuk, J. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints |
| 264 | 1 | |c 2004 | |
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| 520 | |a Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. | ||
| 650 | 4 | |a Theoretical Model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Phase Space |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Detector Efficiency |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Experimental Constraint |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Polarization Observable |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Thörngren Engblom, P. |e verfasserin |4 aut | |
| 700 | 1 | |a Meyer, H.-O. |e verfasserin |4 aut | |
| 700 | 1 | |a Whitaker, T. J. |e verfasserin |4 aut | |
| 700 | 1 | |a Witała, H. |e verfasserin |4 aut | |
| 700 | 1 | |a Golak, J. |e verfasserin |4 aut | |
| 700 | 1 | |a Kamada, H. |e verfasserin |4 aut | |
| 700 | 1 | |a Nogga, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Skibiński, R. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Few-body systems |d Wien [u.a.] : Springer, 1986 |g 34(2004), 4 vom: 28. Mai, Seite 259-273 |w (DE-627)25372323X |w (DE-600)1459107-8 |x 1432-5411 |7 nnns |
| 773 | 1 | 8 | |g volume:34 |g year:2004 |g number:4 |g day:28 |g month:05 |g pages:259-273 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s00601-004-0055-1 |z lizenzpflichtig |3 Volltext |
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| allfields |
10.1007/s00601-004-0055-1 doi (DE-627)SPR007044216 (SPR)s00601-004-0055-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Kuroś-Żołnierczuk, J. verfasserin aut Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints 2004 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. Theoretical Model (dpeaa)DE-He213 Phase Space (dpeaa)DE-He213 Detector Efficiency (dpeaa)DE-He213 Experimental Constraint (dpeaa)DE-He213 Polarization Observable (dpeaa)DE-He213 Thörngren Engblom, P. verfasserin aut Meyer, H.-O. verfasserin aut Whitaker, T. J. verfasserin aut Witała, H. verfasserin aut Golak, J. verfasserin aut Kamada, H. verfasserin aut Nogga, A. verfasserin aut Skibiński, R. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 34(2004), 4 vom: 28. Mai, Seite 259-273 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:34 year:2004 number:4 day:28 month:05 pages:259-273 https://dx.doi.org/10.1007/s00601-004-0055-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4320 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 31.00 ASE 33.00 ASE AR 34 2004 4 28 05 259-273 |
| spelling |
10.1007/s00601-004-0055-1 doi (DE-627)SPR007044216 (SPR)s00601-004-0055-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Kuroś-Żołnierczuk, J. verfasserin aut Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints 2004 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. Theoretical Model (dpeaa)DE-He213 Phase Space (dpeaa)DE-He213 Detector Efficiency (dpeaa)DE-He213 Experimental Constraint (dpeaa)DE-He213 Polarization Observable (dpeaa)DE-He213 Thörngren Engblom, P. verfasserin aut Meyer, H.-O. verfasserin aut Whitaker, T. J. verfasserin aut Witała, H. verfasserin aut Golak, J. verfasserin aut Kamada, H. verfasserin aut Nogga, A. verfasserin aut Skibiński, R. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 34(2004), 4 vom: 28. Mai, Seite 259-273 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:34 year:2004 number:4 day:28 month:05 pages:259-273 https://dx.doi.org/10.1007/s00601-004-0055-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4320 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 31.00 ASE 33.00 ASE AR 34 2004 4 28 05 259-273 |
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10.1007/s00601-004-0055-1 doi (DE-627)SPR007044216 (SPR)s00601-004-0055-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Kuroś-Żołnierczuk, J. verfasserin aut Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints 2004 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. Theoretical Model (dpeaa)DE-He213 Phase Space (dpeaa)DE-He213 Detector Efficiency (dpeaa)DE-He213 Experimental Constraint (dpeaa)DE-He213 Polarization Observable (dpeaa)DE-He213 Thörngren Engblom, P. verfasserin aut Meyer, H.-O. verfasserin aut Whitaker, T. J. verfasserin aut Witała, H. verfasserin aut Golak, J. verfasserin aut Kamada, H. verfasserin aut Nogga, A. verfasserin aut Skibiński, R. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 34(2004), 4 vom: 28. Mai, Seite 259-273 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:34 year:2004 number:4 day:28 month:05 pages:259-273 https://dx.doi.org/10.1007/s00601-004-0055-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4320 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 31.00 ASE 33.00 ASE AR 34 2004 4 28 05 259-273 |
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10.1007/s00601-004-0055-1 doi (DE-627)SPR007044216 (SPR)s00601-004-0055-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Kuroś-Żołnierczuk, J. verfasserin aut Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints 2004 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. Theoretical Model (dpeaa)DE-He213 Phase Space (dpeaa)DE-He213 Detector Efficiency (dpeaa)DE-He213 Experimental Constraint (dpeaa)DE-He213 Polarization Observable (dpeaa)DE-He213 Thörngren Engblom, P. verfasserin aut Meyer, H.-O. verfasserin aut Whitaker, T. J. verfasserin aut Witała, H. verfasserin aut Golak, J. verfasserin aut Kamada, H. verfasserin aut Nogga, A. verfasserin aut Skibiński, R. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 34(2004), 4 vom: 28. Mai, Seite 259-273 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:34 year:2004 number:4 day:28 month:05 pages:259-273 https://dx.doi.org/10.1007/s00601-004-0055-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4320 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 31.00 ASE 33.00 ASE AR 34 2004 4 28 05 259-273 |
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10.1007/s00601-004-0055-1 doi (DE-627)SPR007044216 (SPR)s00601-004-0055-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Kuroś-Żołnierczuk, J. verfasserin aut Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints 2004 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. Theoretical Model (dpeaa)DE-He213 Phase Space (dpeaa)DE-He213 Detector Efficiency (dpeaa)DE-He213 Experimental Constraint (dpeaa)DE-He213 Polarization Observable (dpeaa)DE-He213 Thörngren Engblom, P. verfasserin aut Meyer, H.-O. verfasserin aut Whitaker, T. J. verfasserin aut Witała, H. verfasserin aut Golak, J. verfasserin aut Kamada, H. verfasserin aut Nogga, A. verfasserin aut Skibiński, R. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 34(2004), 4 vom: 28. Mai, Seite 259-273 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:34 year:2004 number:4 day:28 month:05 pages:259-273 https://dx.doi.org/10.1007/s00601-004-0055-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4320 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 31.00 ASE 33.00 ASE AR 34 2004 4 28 05 259-273 |
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Enthalten in Few-body systems 34(2004), 4 vom: 28. Mai, Seite 259-273 volume:34 year:2004 number:4 day:28 month:05 pages:259-273 |
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Enthalten in Few-body systems 34(2004), 4 vom: 28. Mai, Seite 259-273 volume:34 year:2004 number:4 day:28 month:05 pages:259-273 |
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Theoretical Model Phase Space Detector Efficiency Experimental Constraint Polarization Observable |
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Kuroś-Żołnierczuk, J. @@aut@@ Thörngren Engblom, P. @@aut@@ Meyer, H.-O. @@aut@@ Whitaker, T. J. @@aut@@ Witała, H. @@aut@@ Golak, J. @@aut@@ Kamada, H. @@aut@@ Nogga, A. @@aut@@ Skibiński, R. @@aut@@ |
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We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. 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530 ASE 31.00 bkl 33.00 bkl Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints Theoretical Model (dpeaa)DE-He213 Phase Space (dpeaa)DE-He213 Detector Efficiency (dpeaa)DE-He213 Experimental Constraint (dpeaa)DE-He213 Polarization Observable (dpeaa)DE-He213 |
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Kuroś-Żołnierczuk, J. Thörngren Engblom, P. Meyer, H.-O. Whitaker, T. J. Witała, H. Golak, J. Kamada, H. Nogga, A. Skibiński, R. |
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Kuroś-Żołnierczuk, J. |
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10.1007/s00601-004-0055-1 |
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faddeev calculations of breakup reactions with realistic experimental constraints |
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Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints |
| abstract |
Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. |
| abstractGer |
Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. |
| abstract_unstemmed |
Abstract. We present a method to integrate predictions from a theoretical model of a reaction with three bodies in the final state over the region of phase space covered by a given experiment. The method takes into account the true experimental acceptance, as well as variations of detector efficiency, and eliminates the need for a Monte-Carlo simulation of the detector setup. The method is applicable to kinematically complete experiments. Examples for the use of this method include several polarization observables in dp breakup at 270 MeV. The calculations are carried out in the Faddeev framework with the CD Bonn nucleon-nucleon interaction, with or without the inclusion of an additional three-nucleon force. |
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Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints |
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| score |
7.401165 |