Loading…

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...

Full description

Saved in:
Bibliographic Details
Published in:The Astrophysical journal 2013-11, Vol.777 (2)
Main Authors: 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.
Format: Article
Language:English
Subjects:
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by
cites
container_end_page
container_issue 2
container_start_page
container_title The Astrophysical journal
container_volume 777
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
format article
fullrecord <record><control><sourceid>osti</sourceid><recordid>TN_cdi_osti_scitechconnect_22270564</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>22270564</sourcerecordid><originalsourceid>FETCH-LOGICAL-o98t-4aba703fad53b37997f76c08f1cf4bc45a17bebf9cd394fb1d4029cf5ba61d223</originalsourceid><addsrcrecordid>eNo9jd1KwzAAhYMoOKdP4E3AGwVj89emuSxduhW6VNpMvBtN2uBENiH1SvZQvojPJLrh1eE7fJwDwDXBDwSnaYQx5ihh4jkSQkQ0IpydgAmJWYo4i8UpmPwb5-AihNdfpFJOwFhraBYKLlXWrhq1VNrAuvirPsPHOyRsn99-f93D7d2Bk30NW1RkuakbmBmo1Twz5ZOCSqtmXqoWZnoGS9PCUhfVSulcweNHQI9Nnau2vQRnvnsLw9Uxp8AUyuQLVNXzMs8qtJPpiHhnO4GZ7_qYWSakFF4kDqeeOM-t43FHhB2sl65nkntLeo6pdD62XUJ6StkU3Bxmd2HcrIPbjIN7cbvtdnDjmlIqcJxw9gP2g1Xz</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><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><source>Free E-Journal (出版社公開部分のみ)</source><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.</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 ∼&lt; A ∼&lt; 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼&lt; 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><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.1088/0004-637X/777/2/143</identifier><language>eng</language><publisher>United States</publisher><subject>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</subject><ispartof>The Astrophysical journal, 2013-11, Vol.777 (2)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22270564$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>La Cognata, M.</creatorcontrib><creatorcontrib>Spitaleri, C.</creatorcontrib><creatorcontrib>Trippella, O.</creatorcontrib><creatorcontrib>Kiss, G. 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 ∼&lt; A ∼&lt; 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼&lt; 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. G.</creator><creator>Guardo, G. L.</creator><creator>Puglia, S. M. R.</creator><creator>Romano, S.</creator><creator>Spartà, R.</creator><creator>Rogachev, G. V.</creator><creator>Avila, M.</creator><creator>Koshchiy, E.</creator><creator>Kuchera, A.</creator><creator>Santiago, D.</creator><creator>Mukhamedzhanov, A. M.</creator><creator>Lamia, L.</creator><scope>OTOTI</scope></search><sort><creationdate>20131110</creationdate><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><author>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.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o98t-4aba703fad53b37997f76c08f1cf4bc45a17bebf9cd394fb1d4029cf5ba61d223</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>ALPHA REACTIONS</topic><topic>ASTROPHYSICS</topic><topic>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</topic><topic>ASYMPTOTIC SOLUTIONS</topic><topic>CARBON 13 TARGET</topic><topic>CARBON 17</topic><topic>COMPARATIVE EVALUATIONS</topic><topic>HELIUM BURNING</topic><topic>KEV RANGE</topic><topic>LITHIUM 6 REACTIONS</topic><topic>MEV RANGE</topic><topic>NUCLEAR PHYSICS AND RADIATION PHYSICS</topic><topic>NUCLEOSYNTHESIS</topic><topic>OXYGEN 16</topic><topic>OXYGEN 17</topic><topic>QUASI-FREE REACTIONS</topic><topic>R MATRIX</topic><topic>S PROCESS</topic><topic>STARS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>La Cognata, M.</creatorcontrib><creatorcontrib>Spitaleri, C.</creatorcontrib><creatorcontrib>Trippella, O.</creatorcontrib><creatorcontrib>Kiss, G. 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 ∼&lt; A ∼&lt; 208. This reaction takes place inside the helium-burning shell of asymptotic giant branch stars, at temperatures ∼&lt; 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>
fulltext fulltext
identifier ISSN: 0004-637X
ispartof The Astrophysical journal, 2013-11, Vol.777 (2)
issn 0004-637X
1538-4357
language eng
recordid cdi_osti_scitechconnect_22270564
source Free E-Journal (出版社公開部分のみ)
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
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-01T05%3A33%3A05IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-osti&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=ON%20THE%20MEASUREMENT%20OF%20THE%20%7Bsup%2013%7DC(%CE%B1,%20n)%7Bsup%2016%7DO%20S-FACTOR%20AT%20NEGATIVE%20ENERGIES%20AND%20ITS%20INFLUENCE%20ON%20THE%20s-PROCESS&rft.jtitle=The%20Astrophysical%20journal&rft.au=La%20Cognata,%20M.&rft.date=2013-11-10&rft.volume=777&rft.issue=2&rft.issn=0004-637X&rft.eissn=1538-4357&rft_id=info:doi/10.1088/0004-637X/777/2/143&rft_dat=%3Costi%3E22270564%3C/osti%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-o98t-4aba703fad53b37997f76c08f1cf4bc45a17bebf9cd394fb1d4029cf5ba61d223%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true