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ON THE MEASUREMENT OF THE {sup 13}C(α, n){sup 16}O S-FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s-PROCESS
The {sup 13}C(α, n){sup 16}O reaction is the neutron source for the main component of the s-process, responsible for the production of most of the nuclei in the mass range 90 ∼< A ∼< 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperature...
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Published in: | The Astrophysical journal 2013-11, Vol.777 (2) |
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creator | La Cognata, M. Spitaleri, C. Trippella, O. Kiss, G. G. Guardo, G. L. Puglia, S. M. R. Romano, S. Spartà, R. Rogachev, G. V. Avila, M. Koshchiy, E. Kuchera, A. Santiago, D. Mukhamedzhanov, A. M. Lamia, L. |
description | The {sup 13}C(α, n){sup 16}O reaction is the neutron source for the main component of the s-process, responsible for the production of most of the nuclei in the mass range 90 ∼< A ∼< 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼< 10{sup 8} K, corresponding to an energy interval where the {sup 13}C(α, n){sup 16}O reaction is effective in the range of 140-230 keV. In this regime, the astrophysical S(E)-factor is dominated by the –3 keV sub-threshold resonance due to the 6.356 MeV level in {sup 17}O, giving rise to a steep increase in the S-factor. Its contribution is still controversial as extrapolations, e.g., through the R-matrix and indirect techniques such as the asymptotic normalization coefficient (ANC), yield inconsistent results. The discrepancy amounts to a factor of three or more precisely at astrophysical energies. To provide a more accurate S-factor at these energies, we have applied the Trojan horse method (THM) to the {sup 13}C({sup 6}Li, n {sup 16}O)d quasi-free reaction. The ANC for the 6.356 MeV level has been deduced through the THM as well as the n-partial width, allowing us to attain unprecedented accuracy for the {sup 13}C(α, n){sup 16}O astrophysical factor. A larger ANC for the 6.356 MeV level is measured with respect to the ones in the literature, (C-tilde{sub α{sup 1}{sup 3}C}{sup 17O(1/2+)2} = 7.7 ± 0.3{sub stat} {sub -1.5}{sup +1.}|6 norm fm{sup –1}, yet in agreement with the preliminary result given in our preceding letter, indicating an increase of the {sup 13}C(α, n){sup 16}O reaction rate below about 8 × 10{sup 7} K if compared with the recommended values. At ∼10{sup 8} K, our reaction rate agrees with most of the results in the literature and the accuracy is greatly enhanced thanks to this innovative approach. |
doi_str_mv | 10.1088/0004-637X/777/2/143 |
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G. ; Guardo, G. L. ; Puglia, S. M. R. ; Romano, S. ; Spartà, R. ; Rogachev, G. V. ; Avila, M. ; Koshchiy, E. ; Kuchera, A. ; Santiago, D. ; Mukhamedzhanov, A. M. ; Lamia, L.</creator><creatorcontrib>La Cognata, M. ; Spitaleri, C. ; Trippella, O. ; Kiss, G. G. ; Guardo, G. L. ; Puglia, S. M. R. ; Romano, S. ; Spartà, R. ; Rogachev, G. V. ; Avila, M. ; Koshchiy, E. ; Kuchera, A. ; Santiago, D. ; Mukhamedzhanov, A. M. ; Lamia, L.</creatorcontrib><description>The {sup 13}C(α, n){sup 16}O reaction is the neutron source for the main component of the s-process, responsible for the production of most of the nuclei in the mass range 90 ∼< A ∼< 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼< 10{sup 8} K, corresponding to an energy interval where the {sup 13}C(α, n){sup 16}O reaction is effective in the range of 140-230 keV. In this regime, the astrophysical S(E)-factor is dominated by the –3 keV sub-threshold resonance due to the 6.356 MeV level in {sup 17}O, giving rise to a steep increase in the S-factor. Its contribution is still controversial as extrapolations, e.g., through the R-matrix and indirect techniques such as the asymptotic normalization coefficient (ANC), yield inconsistent results. The discrepancy amounts to a factor of three or more precisely at astrophysical energies. To provide a more accurate S-factor at these energies, we have applied the Trojan horse method (THM) to the {sup 13}C({sup 6}Li, n {sup 16}O)d quasi-free reaction. The ANC for the 6.356 MeV level has been deduced through the THM as well as the n-partial width, allowing us to attain unprecedented accuracy for the {sup 13}C(α, n){sup 16}O astrophysical factor. A larger ANC for the 6.356 MeV level is measured with respect to the ones in the literature, (C-tilde{sub α{sup 1}{sup 3}C}{sup 17O(1/2+)2} = 7.7 ± 0.3{sub stat} {sub -1.5}{sup +1.}|6 norm fm{sup –1}, yet in agreement with the preliminary result given in our preceding letter, indicating an increase of the {sup 13}C(α, n){sup 16}O reaction rate below about 8 × 10{sup 7} K if compared with the recommended values. 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G.</creatorcontrib><creatorcontrib>Guardo, G. L.</creatorcontrib><creatorcontrib>Puglia, S. M. R.</creatorcontrib><creatorcontrib>Romano, S.</creatorcontrib><creatorcontrib>Spartà, R.</creatorcontrib><creatorcontrib>Rogachev, G. V.</creatorcontrib><creatorcontrib>Avila, M.</creatorcontrib><creatorcontrib>Koshchiy, E.</creatorcontrib><creatorcontrib>Kuchera, A.</creatorcontrib><creatorcontrib>Santiago, D.</creatorcontrib><creatorcontrib>Mukhamedzhanov, A. M.</creatorcontrib><creatorcontrib>Lamia, L.</creatorcontrib><title>ON THE MEASUREMENT OF THE {sup 13}C(α, n){sup 16}O S-FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s-PROCESS</title><title>The Astrophysical journal</title><description>The {sup 13}C(α, n){sup 16}O reaction is the neutron source for the main component of the s-process, responsible for the production of most of the nuclei in the mass range 90 ∼< A ∼< 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼< 10{sup 8} K, corresponding to an energy interval where the {sup 13}C(α, n){sup 16}O reaction is effective in the range of 140-230 keV. In this regime, the astrophysical S(E)-factor is dominated by the –3 keV sub-threshold resonance due to the 6.356 MeV level in {sup 17}O, giving rise to a steep increase in the S-factor. Its contribution is still controversial as extrapolations, e.g., through the R-matrix and indirect techniques such as the asymptotic normalization coefficient (ANC), yield inconsistent results. The discrepancy amounts to a factor of three or more precisely at astrophysical energies. To provide a more accurate S-factor at these energies, we have applied the Trojan horse method (THM) to the {sup 13}C({sup 6}Li, n {sup 16}O)d quasi-free reaction. The ANC for the 6.356 MeV level has been deduced through the THM as well as the n-partial width, allowing us to attain unprecedented accuracy for the {sup 13}C(α, n){sup 16}O astrophysical factor. A larger ANC for the 6.356 MeV level is measured with respect to the ones in the literature, (C-tilde{sub α{sup 1}{sup 3}C}{sup 17O(1/2+)2} = 7.7 ± 0.3{sub stat} {sub -1.5}{sup +1.}|6 norm fm{sup –1}, yet in agreement with the preliminary result given in our preceding letter, indicating an increase of the {sup 13}C(α, n){sup 16}O reaction rate below about 8 × 10{sup 7} K if compared with the recommended values. At ∼10{sup 8} K, our reaction rate agrees with most of the results in the literature and the accuracy is greatly enhanced thanks to this innovative approach.</description><subject>ALPHA REACTIONS</subject><subject>ASTROPHYSICS</subject><subject>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</subject><subject>ASYMPTOTIC SOLUTIONS</subject><subject>CARBON 13 TARGET</subject><subject>CARBON 17</subject><subject>COMPARATIVE EVALUATIONS</subject><subject>HELIUM BURNING</subject><subject>KEV RANGE</subject><subject>LITHIUM 6 REACTIONS</subject><subject>MEV RANGE</subject><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><subject>NUCLEOSYNTHESIS</subject><subject>OXYGEN 16</subject><subject>OXYGEN 17</subject><subject>QUASI-FREE REACTIONS</subject><subject>R MATRIX</subject><subject>S PROCESS</subject><subject>STARS</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNo9jd1KwzAAhYMoOKdP4E3AGwVj89emuSxduhW6VNpMvBtN2uBENiH1SvZQvojPJLrh1eE7fJwDwDXBDwSnaYQx5ihh4jkSQkQ0IpydgAmJWYo4i8UpmPwb5-AihNdfpFJOwFhraBYKLlXWrhq1VNrAuvirPsPHOyRsn99-f93D7d2Bk30NW1RkuakbmBmo1Twz5ZOCSqtmXqoWZnoGS9PCUhfVSulcweNHQI9Nnau2vQRnvnsLw9Uxp8AUyuQLVNXzMs8qtJPpiHhnO4GZ7_qYWSakFF4kDqeeOM-t43FHhB2sl65nkntLeo6pdD62XUJ6StkU3Bxmd2HcrIPbjIN7cbvtdnDjmlIqcJxw9gP2g1Xz</recordid><startdate>20131110</startdate><enddate>20131110</enddate><creator>La Cognata, M.</creator><creator>Spitaleri, C.</creator><creator>Trippella, O.</creator><creator>Kiss, G. 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G.</creatorcontrib><creatorcontrib>Guardo, G. L.</creatorcontrib><creatorcontrib>Puglia, S. M. R.</creatorcontrib><creatorcontrib>Romano, S.</creatorcontrib><creatorcontrib>Spartà, R.</creatorcontrib><creatorcontrib>Rogachev, G. V.</creatorcontrib><creatorcontrib>Avila, M.</creatorcontrib><creatorcontrib>Koshchiy, E.</creatorcontrib><creatorcontrib>Kuchera, A.</creatorcontrib><creatorcontrib>Santiago, D.</creatorcontrib><creatorcontrib>Mukhamedzhanov, A. M.</creatorcontrib><creatorcontrib>Lamia, L.</creatorcontrib><collection>OSTI.GOV</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>La Cognata, M.</au><au>Spitaleri, C.</au><au>Trippella, O.</au><au>Kiss, G. G.</au><au>Guardo, G. L.</au><au>Puglia, S. M. R.</au><au>Romano, S.</au><au>Spartà, R.</au><au>Rogachev, G. V.</au><au>Avila, M.</au><au>Koshchiy, E.</au><au>Kuchera, A.</au><au>Santiago, D.</au><au>Mukhamedzhanov, A. M.</au><au>Lamia, L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>ON THE MEASUREMENT OF THE {sup 13}C(α, n){sup 16}O S-FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s-PROCESS</atitle><jtitle>The Astrophysical journal</jtitle><date>2013-11-10</date><risdate>2013</risdate><volume>777</volume><issue>2</issue><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>The {sup 13}C(α, n){sup 16}O reaction is the neutron source for the main component of the s-process, responsible for the production of most of the nuclei in the mass range 90 ∼< A ∼< 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼< 10{sup 8} K, corresponding to an energy interval where the {sup 13}C(α, n){sup 16}O reaction is effective in the range of 140-230 keV. In this regime, the astrophysical S(E)-factor is dominated by the –3 keV sub-threshold resonance due to the 6.356 MeV level in {sup 17}O, giving rise to a steep increase in the S-factor. Its contribution is still controversial as extrapolations, e.g., through the R-matrix and indirect techniques such as the asymptotic normalization coefficient (ANC), yield inconsistent results. The discrepancy amounts to a factor of three or more precisely at astrophysical energies. To provide a more accurate S-factor at these energies, we have applied the Trojan horse method (THM) to the {sup 13}C({sup 6}Li, n {sup 16}O)d quasi-free reaction. The ANC for the 6.356 MeV level has been deduced through the THM as well as the n-partial width, allowing us to attain unprecedented accuracy for the {sup 13}C(α, n){sup 16}O astrophysical factor. A larger ANC for the 6.356 MeV level is measured with respect to the ones in the literature, (C-tilde{sub α{sup 1}{sup 3}C}{sup 17O(1/2+)2} = 7.7 ± 0.3{sub stat} {sub -1.5}{sup +1.}|6 norm fm{sup –1}, yet in agreement with the preliminary result given in our preceding letter, indicating an increase of the {sup 13}C(α, n){sup 16}O reaction rate below about 8 × 10{sup 7} K if compared with the recommended values. At ∼10{sup 8} K, our reaction rate agrees with most of the results in the literature and the accuracy is greatly enhanced thanks to this innovative approach.</abstract><cop>United States</cop><doi>10.1088/0004-637X/777/2/143</doi></addata></record> |
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subjects | ALPHA REACTIONS ASTROPHYSICS ASTROPHYSICS, COSMOLOGY AND ASTRONOMY ASYMPTOTIC SOLUTIONS CARBON 13 TARGET CARBON 17 COMPARATIVE EVALUATIONS HELIUM BURNING KEV RANGE LITHIUM 6 REACTIONS MEV RANGE NUCLEAR PHYSICS AND RADIATION PHYSICS NUCLEOSYNTHESIS OXYGEN 16 OXYGEN 17 QUASI-FREE REACTIONS R MATRIX S PROCESS STARS |
title | ON THE MEASUREMENT OF THE {sup 13}C(α, n){sup 16}O S-FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s-PROCESS |
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