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dc.contributor.author한인식*
dc.date.accessioned2016-08-27T04:08:55Z-
dc.date.available2016-08-27T04:08:55Z-
dc.date.issued2014*
dc.identifier.issn0556-2813*
dc.identifier.issn1089-490X*
dc.identifier.otherOAK-11818*
dc.identifier.urihttps://dspace.ewha.ac.kr/handle/2015.oak/216883-
dc.description.abstractThe O-14(alpha, p)F-17 reaction is one of the key reactions involved in the breakout from the hot-CNO cycle to the rp-process in type-I x-ray bursts (XRBs). The resonant properties in the compound nucleus Ne-18 have been investigated through resonant elastic scattering of F-17 + p. The radioactive F-17 beam was separated by the Center for Nuclear Study radioactive ion beam separator (CRIB) and bombarded a thick H-2 gas target at 3.6 MeV/nucleon. The recoiling light particles were measured by three Delta E-E silicon telescopes at laboratory angles of theta(lab) approximate to 3 degrees, 10 degrees, and 18 degrees. Five resonances at E-x = 6.15, 6.28, 6.35, 6.85, and 7.05 MeV were observed in the excitation functions, and their spin-parities have been determined based on an R-matrix analysis. In particular, J(pi) = 1(-) was firmly assigned to the 6.15-MeV state which dominates the thermonuclear O-14(alpha, p)F-17 rate below 2 GK. As well, a possible new excited state in Ne-18 was observed at E-x = 6.85 +/- 0.11 MeV with tentative J = 0 assignment. This state could be the analog state of the 6.880 MeV (0(-)) level in the mirror nucleus O-18, or a bandhead state (0(+)) of the six-particle four-hole (6p-4h) band. A new thermonuclear O-14(alpha, p)F-17 rate has been determined, and the astrophysical impact of multiple recent rates has been examined using an XRB model. Contrary to previous expectations, we find only a modest impact on predicted nuclear energy generation rates from using reaction rates differing by up to several orders of magnitude.*
dc.languageEnglish*
dc.publisherAMER PHYSICAL SOC*
dc.titleExamination of the role of the O-14(alpha, p)F-17 reaction rate in type-I x-ray bursts*
dc.typeArticle*
dc.relation.issue2*
dc.relation.volume90*
dc.relation.indexSCI*
dc.relation.indexSCIE*
dc.relation.indexSCOPUS*
dc.relation.journaltitlePHYSICAL REVIEW C*
dc.identifier.doi10.1103/PhysRevC.90.025803*
dc.identifier.wosidWOS:000341240300005*
dc.author.googleHu, J.*
dc.author.googleHe, J. J.*
dc.author.googleParikh, A.*
dc.author.googleXu, S. W.*
dc.author.googleYamaguchi, H.*
dc.author.googleKahl, D.*
dc.author.googleMa, P.*
dc.author.googleSu, J.*
dc.author.googleWang, H. W.*
dc.author.googleNakao, T.*
dc.author.googleWakabayashi, Y.*
dc.author.googleTeranishi, T.*
dc.author.googleHahn, K. I.*
dc.author.googleMoon, J. Y.*
dc.author.googleJung, H. S.*
dc.author.googleHashimoto, T.*
dc.author.googleChen, A. A.*
dc.author.googleIrvine, D.*
dc.author.googleLee, C. S.*
dc.author.googleKubono, S.*
dc.contributor.scopusid한인식(7201832280;57205469686;57192312712)*
dc.date.modifydate20240415134453*


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