Fusion of 60Ni + 100Mo near and below the Coulomb barrier
Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Stefanini, A. M. [verfasserIn] Montagnoli, G. [verfasserIn] Scarlassara, F. [verfasserIn] Jiang, C. L. [verfasserIn] Esbensen, H. [verfasserIn] Fioretto, E. [verfasserIn] Corradi, L. [verfasserIn] Back, B. B. [verfasserIn] Deibel, C. M. [verfasserIn] Di Giovine, B. [verfasserIn] Greene, J. P. [verfasserIn] Henderson, H. D. [verfasserIn] Marley, S. T. [verfasserIn] Notani, M. [verfasserIn] Patel, N. [verfasserIn] Rehm, K. E. [verfasserIn] Sewerinyak, D. [verfasserIn] Tang, X. D. [verfasserIn] Ugalde, C. [verfasserIn] Zhu, S. [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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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 49(2013), 5 vom: 27. Mai |
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| Übergeordnetes Werk: |
volume:49 ; year:2013 ; number:5 ; day:27 ; month:05 |
| Links: |
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| DOI / URN: |
10.1140/epja/i2013-13063-2 |
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| Katalog-ID: |
SPR008280797 |
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| 100 | 1 | |a Stefanini, A. M. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Fusion of 60Ni + 100Mo near and below the Coulomb barrier |
| 264 | 1 | |c 2013 | |
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| 520 | |a Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. | ||
| 650 | 4 | |a Excitation Function |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Coulomb Barrier |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Fusion Cross Section |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Evaporation Residue |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Molybdenum Isotope |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Montagnoli, G. |e verfasserin |4 aut | |
| 700 | 1 | |a Scarlassara, F. |e verfasserin |4 aut | |
| 700 | 1 | |a Jiang, C. L. |e verfasserin |4 aut | |
| 700 | 1 | |a Esbensen, H. |e verfasserin |4 aut | |
| 700 | 1 | |a Fioretto, E. |e verfasserin |4 aut | |
| 700 | 1 | |a Corradi, L. |e verfasserin |4 aut | |
| 700 | 1 | |a Back, B. B. |e verfasserin |4 aut | |
| 700 | 1 | |a Deibel, C. M. |e verfasserin |4 aut | |
| 700 | 1 | |a Di Giovine, B. |e verfasserin |4 aut | |
| 700 | 1 | |a Greene, J. P. |e verfasserin |4 aut | |
| 700 | 1 | |a Henderson, H. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Marley, S. T. |e verfasserin |4 aut | |
| 700 | 1 | |a Notani, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Patel, N. |e verfasserin |4 aut | |
| 700 | 1 | |a Rehm, K. E. |e verfasserin |4 aut | |
| 700 | 1 | |a Sewerinyak, D. |e verfasserin |4 aut | |
| 700 | 1 | |a Tang, X. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Ugalde, C. |e verfasserin |4 aut | |
| 700 | 1 | |a Zhu, S. |e verfasserin |4 aut | |
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10.1140/epja/i2013-13063-2 doi (DE-627)SPR008280797 (SPR)i2013-13063-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Stefanini, A. M. verfasserin aut Fusion of 60Ni + 100Mo near and below the Coulomb barrier 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. Excitation Function (dpeaa)DE-He213 Coulomb Barrier (dpeaa)DE-He213 Fusion Cross Section (dpeaa)DE-He213 Evaporation Residue (dpeaa)DE-He213 Molybdenum Isotope (dpeaa)DE-He213 Montagnoli, G. verfasserin aut Scarlassara, F. verfasserin aut Jiang, C. L. verfasserin aut Esbensen, H. verfasserin aut Fioretto, E. verfasserin aut Corradi, L. verfasserin aut Back, B. B. verfasserin aut Deibel, C. M. verfasserin aut Di Giovine, B. verfasserin aut Greene, J. P. verfasserin aut Henderson, H. D. verfasserin aut Marley, S. T. verfasserin aut Notani, M. verfasserin aut Patel, N. verfasserin aut Rehm, K. E. verfasserin aut Sewerinyak, D. verfasserin aut Tang, X. D. verfasserin aut Ugalde, C. verfasserin aut Zhu, S. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 49(2013), 5 vom: 27. Mai (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:49 year:2013 number:5 day:27 month:05 https://dx.doi.org/10.1140/epja/i2013-13063-2 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_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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_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 33.40 ASE 33.50 ASE AR 49 2013 5 27 05 |
| spelling |
10.1140/epja/i2013-13063-2 doi (DE-627)SPR008280797 (SPR)i2013-13063-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Stefanini, A. M. verfasserin aut Fusion of 60Ni + 100Mo near and below the Coulomb barrier 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. Excitation Function (dpeaa)DE-He213 Coulomb Barrier (dpeaa)DE-He213 Fusion Cross Section (dpeaa)DE-He213 Evaporation Residue (dpeaa)DE-He213 Molybdenum Isotope (dpeaa)DE-He213 Montagnoli, G. verfasserin aut Scarlassara, F. verfasserin aut Jiang, C. L. verfasserin aut Esbensen, H. verfasserin aut Fioretto, E. verfasserin aut Corradi, L. verfasserin aut Back, B. B. verfasserin aut Deibel, C. M. verfasserin aut Di Giovine, B. verfasserin aut Greene, J. P. verfasserin aut Henderson, H. D. verfasserin aut Marley, S. T. verfasserin aut Notani, M. verfasserin aut Patel, N. verfasserin aut Rehm, K. E. verfasserin aut Sewerinyak, D. verfasserin aut Tang, X. D. verfasserin aut Ugalde, C. verfasserin aut Zhu, S. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 49(2013), 5 vom: 27. Mai (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:49 year:2013 number:5 day:27 month:05 https://dx.doi.org/10.1140/epja/i2013-13063-2 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_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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_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 33.40 ASE 33.50 ASE AR 49 2013 5 27 05 |
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10.1140/epja/i2013-13063-2 doi (DE-627)SPR008280797 (SPR)i2013-13063-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Stefanini, A. M. verfasserin aut Fusion of 60Ni + 100Mo near and below the Coulomb barrier 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. Excitation Function (dpeaa)DE-He213 Coulomb Barrier (dpeaa)DE-He213 Fusion Cross Section (dpeaa)DE-He213 Evaporation Residue (dpeaa)DE-He213 Molybdenum Isotope (dpeaa)DE-He213 Montagnoli, G. verfasserin aut Scarlassara, F. verfasserin aut Jiang, C. L. verfasserin aut Esbensen, H. verfasserin aut Fioretto, E. verfasserin aut Corradi, L. verfasserin aut Back, B. B. verfasserin aut Deibel, C. M. verfasserin aut Di Giovine, B. verfasserin aut Greene, J. P. verfasserin aut Henderson, H. D. verfasserin aut Marley, S. T. verfasserin aut Notani, M. verfasserin aut Patel, N. verfasserin aut Rehm, K. E. verfasserin aut Sewerinyak, D. verfasserin aut Tang, X. D. verfasserin aut Ugalde, C. verfasserin aut Zhu, S. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 49(2013), 5 vom: 27. Mai (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:49 year:2013 number:5 day:27 month:05 https://dx.doi.org/10.1140/epja/i2013-13063-2 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_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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_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 33.40 ASE 33.50 ASE AR 49 2013 5 27 05 |
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10.1140/epja/i2013-13063-2 doi (DE-627)SPR008280797 (SPR)i2013-13063-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Stefanini, A. M. verfasserin aut Fusion of 60Ni + 100Mo near and below the Coulomb barrier 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. Excitation Function (dpeaa)DE-He213 Coulomb Barrier (dpeaa)DE-He213 Fusion Cross Section (dpeaa)DE-He213 Evaporation Residue (dpeaa)DE-He213 Molybdenum Isotope (dpeaa)DE-He213 Montagnoli, G. verfasserin aut Scarlassara, F. verfasserin aut Jiang, C. L. verfasserin aut Esbensen, H. verfasserin aut Fioretto, E. verfasserin aut Corradi, L. verfasserin aut Back, B. B. verfasserin aut Deibel, C. M. verfasserin aut Di Giovine, B. verfasserin aut Greene, J. P. verfasserin aut Henderson, H. D. verfasserin aut Marley, S. T. verfasserin aut Notani, M. verfasserin aut Patel, N. verfasserin aut Rehm, K. E. verfasserin aut Sewerinyak, D. verfasserin aut Tang, X. D. verfasserin aut Ugalde, C. verfasserin aut Zhu, S. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 49(2013), 5 vom: 27. Mai (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:49 year:2013 number:5 day:27 month:05 https://dx.doi.org/10.1140/epja/i2013-13063-2 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_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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_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 33.40 ASE 33.50 ASE AR 49 2013 5 27 05 |
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10.1140/epja/i2013-13063-2 doi (DE-627)SPR008280797 (SPR)i2013-13063-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Stefanini, A. M. verfasserin aut Fusion of 60Ni + 100Mo near and below the Coulomb barrier 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. Excitation Function (dpeaa)DE-He213 Coulomb Barrier (dpeaa)DE-He213 Fusion Cross Section (dpeaa)DE-He213 Evaporation Residue (dpeaa)DE-He213 Molybdenum Isotope (dpeaa)DE-He213 Montagnoli, G. verfasserin aut Scarlassara, F. verfasserin aut Jiang, C. L. verfasserin aut Esbensen, H. verfasserin aut Fioretto, E. verfasserin aut Corradi, L. verfasserin aut Back, B. B. verfasserin aut Deibel, C. M. verfasserin aut Di Giovine, B. verfasserin aut Greene, J. P. verfasserin aut Henderson, H. D. verfasserin aut Marley, S. T. verfasserin aut Notani, M. verfasserin aut Patel, N. verfasserin aut Rehm, K. E. verfasserin aut Sewerinyak, D. verfasserin aut Tang, X. D. verfasserin aut Ugalde, C. verfasserin aut Zhu, S. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 49(2013), 5 vom: 27. Mai (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:49 year:2013 number:5 day:27 month:05 https://dx.doi.org/10.1140/epja/i2013-13063-2 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_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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_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 33.40 ASE 33.50 ASE AR 49 2013 5 27 05 |
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Excitation Function Coulomb Barrier Fusion Cross Section Evaporation Residue Molybdenum Isotope |
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Stefanini, A. M. @@aut@@ Montagnoli, G. @@aut@@ Scarlassara, F. @@aut@@ Jiang, C. L. @@aut@@ Esbensen, H. @@aut@@ Fioretto, E. @@aut@@ Corradi, L. @@aut@@ Back, B. B. @@aut@@ Deibel, C. M. @@aut@@ Di Giovine, B. @@aut@@ Greene, J. P. @@aut@@ Henderson, H. D. @@aut@@ Marley, S. T. @@aut@@ Notani, M. @@aut@@ Patel, N. @@aut@@ Rehm, K. E. @@aut@@ Sewerinyak, D. @@aut@@ Tang, X. D. @@aut@@ Ugalde, C. @@aut@@ Zhu, S. @@aut@@ |
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M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Fusion of 60Ni + 100Mo near and below the Coulomb barrier</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2013</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 The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. 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|
| author |
Stefanini, A. M. |
| spellingShingle |
Stefanini, A. M. ddc 530 bkl 33.40 bkl 33.50 misc Excitation Function misc Coulomb Barrier misc Fusion Cross Section misc Evaporation Residue misc Molybdenum Isotope Fusion of 60Ni + 100Mo near and below the Coulomb barrier |
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Stefanini, A. M. |
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electronic Article |
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530 - Physics |
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Not Illustrated |
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530 ASE 33.40 bkl 33.50 bkl Fusion of 60Ni + 100Mo near and below the Coulomb barrier Excitation Function (dpeaa)DE-He213 Coulomb Barrier (dpeaa)DE-He213 Fusion Cross Section (dpeaa)DE-He213 Evaporation Residue (dpeaa)DE-He213 Molybdenum Isotope (dpeaa)DE-He213 |
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ddc 530 bkl 33.40 bkl 33.50 misc Excitation Function misc Coulomb Barrier misc Fusion Cross Section misc Evaporation Residue misc Molybdenum Isotope |
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ddc 530 bkl 33.40 bkl 33.50 misc Excitation Function misc Coulomb Barrier misc Fusion Cross Section misc Evaporation Residue misc Molybdenum Isotope |
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ddc 530 bkl 33.40 bkl 33.50 misc Excitation Function misc Coulomb Barrier misc Fusion Cross Section misc Evaporation Residue misc Molybdenum Isotope |
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Fusion of 60Ni + 100Mo near and below the Coulomb barrier |
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Fusion of 60Ni + 100Mo near and below the Coulomb barrier |
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Stefanini, A. M. |
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Stefanini, A. M. Montagnoli, G. Scarlassara, F. Jiang, C. L. Esbensen, H. Fioretto, E. Corradi, L. Back, B. B. Deibel, C. M. Di Giovine, B. Greene, J. P. Henderson, H. D. Marley, S. T. Notani, M. Patel, N. Rehm, K. E. Sewerinyak, D. Tang, X. D. Ugalde, C. Zhu, S. |
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Stefanini, A. M. |
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10.1140/epja/i2013-13063-2 |
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fusion of 60ni + 100mo near and below the coulomb barrier |
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Fusion of 60Ni + 100Mo near and below the Coulomb barrier |
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Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. |
| abstractGer |
Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. |
| abstract_unstemmed |
Abstract The fusion excitation function of 60Ni + 100Mo has been measured from above the Coulomb barrier down to a cross section around 2 μb, looking for coupling and hindrance effects in this soft medium-mass system with positive Q-values for several neutron transfer channels. A comparison is made with previous results for 64Ni + 100Mo where no Q > 0 transfer channels exist and the hindrance effect is quite clear. The two excitation functions are very similar, as well as the corresponding logarithmic derivatives showing analogous saturations below the barrier. It appears that transfer couplings to Q > 0 channels seem to play a marginal role near and below the barrier for 60Ni + 100Mo , even if measurements of cross sections lower than 1 μb would be needed also for this system. Coupled-channels calculations confirm these observations and indicate that multi-phonon excitations dominate the fusion dynamics in the whole measured energy range. |
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Fusion of 60Ni + 100Mo near and below the Coulomb barrier |
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Montagnoli, G. Scarlassara, F. Jiang, C. L. Esbensen, H. Fioretto, E. Corradi, L. Back, B. B. Deibel, C. M. Di Giovine, B. Greene, J. P. Henderson, H. D. Marley, S. T. Notani, M. Patel, N. Rehm, K. E. Sewerinyak, D. Tang, X. D. Ugalde, C. Zhu, S. |
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| score |
7.4014053 |