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Determination of the astrophysical factor of the <sup>3</sup>He(α,γ)<sup>7</sup>Be down to zero energy using the asymptotic normalization coefficient method

M. La CognataLaboratori Nazionali del Sud - INFN, Via S. Sofia 62, 95123 Catania, ItalyG. KissInstitute for Nuclear Research (ATOMKI), H-4001 Debrecen, POB.51, HungaryR. YarmukhamedovInstitute of Nuclear Physics, Uzbekistan Academy of Sciences, 100214 Tashkent, UzbekistanK. I. TursunmakhatovInstitute of Nuclear Physics, Uzbekistan Academy of Sciences, 100214 Tashkent, UzbekistanI. WiedenhöverDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAL. T. BabyDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAS. CherubiniDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyA. CvetinovićJožef Stefan Institute, Department of Low and Medium Energy Physics (F2), 1000 Ljubljana, SloveniaG. D’AgataLaboratori Nazionali del Sud - INFN, Via S. Sofia 62, 95123 Catania, ItalyP. FigueraLaboratori Nazionali del Sud - INFN, Via S. Sofia 62, 95123 Catania, ItalyG. L. GuardoLaboratori Nazionali del Sud - INFN, Via S. Sofia 62, 95123 Catania, ItalyM. GulinoFacoltá di Ingegneria e Architettura, Università di Enna “Kore”, 94100, Enna, ItalyS. HayakawaCenter for Nuclear Study (CNS), University of Tokyo, RIKEN campus, Saitama 351-0198, JapanI. IndelicatoDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyL. LamiaCentro Siciliano di Fisica Nucleare e Struttura della Materia (CSFNSM), Catania 95123, ItalyМ. ЛаттуадаDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyF. MudòDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyS. PalmeriniDipartimento di Fisica e Geologia, Università di Perugia, 06123 Perugia, ItalyR. G. PizzoneDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyG. G. RapisardaDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyS. RomanoCentro Siciliano di Fisica Nucleare e Struttura della Materia (CSFNSM), Catania 95123, ItalyM. L. SergiDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyR. SpartáDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyC. SpitaleriDipartimento di Fisica e Astronomia “E. Majorana”, Università di Catania, 95123 Catania, ItalyO. TrippellaDipartimento di Fisica e Geologia, Università di Perugia, 06123 Perugia, ItalyА. ТуміноFacoltá di Ingegneria e Architettura, Università di Enna “Kore”, 94100, Enna, ItalyM. AnastasiouDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAS. A. KuvinDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAN. RijalDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAB. SchmidtDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAS. B. IgamovInstitute of Nuclear Physics, Uzbekistan Academy of Sciences, 100214 Tashkent, UzbekistanS.B. SakutaNational Research Center “Kurchatov Institute”, Moscow 123182, RussiaZs. FülöpInstitute for Nuclear Research (ATOMKI), H-4001 Debrecen, POB.51, HungaryGy. GyürkyInstitute for Nuclear Research (ATOMKI), H-4001 Debrecen, POB.51, HungaryT. SzücsInstitute for Nuclear Research (ATOMKI), H-4001 Debrecen, POB.51, HungaryZ. HalászInstitute for Nuclear Research (ATOMKI), H-4001 Debrecen, POB.51, HungaryE. SomorjaiInstitute for Nuclear Research (ATOMKI), H-4001 Debrecen, POB.51, HungaryZ. HonsNuclear Physics Institute of the Czech Academy of Sciences, 250 68 Řež, Czech RepublicJ. MrázekNuclear Physics Institute of the Czech Academy of Sciences, 250 68 Řež, Czech RepublicR. E. TribbleCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAA. M. MukhamedzhanovCyclotron Institute, Texas A&M University, College Station, Texas 77843, USA
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Аннотация

Abstract The observation of neutrinos emitted in the p − p chain and in the CNO cycle can be employed to test the Standard Solar Model. The 3 He( α,γ ) 7 Be reaction is the first reaction of the 2nd and 3rd branch of the p − p chain, so the indetermination of its cross section significantly affects the predicted 7 Be and 8 B neutrino fluxes. Notwithstanding its relevance and the great deal of experimental and theoretical papers, information of the reaction cross section at energies of the core of the Sun (15 keV - 30 keV) is sparse and additional experimental work is necessary to attain the target (~ 3%) accuracy. The precise understanding of the external capture component to the 3 He( α,γ ) 7 Be reaction cross section is pivotal for the theoretical assessment of the reaction mechanism. In this work, the indirect measurement of this external capture component using the Asymptotic Normalization Coefficient (ANC) technique is discussed. To extract the ANC, the angular distributions of deuterons yielded in the 6 Li( 3 He, d ) 7 Be α -transfer reaction were detected with high precision at E 3 He =3.0 MeV and 5.0 MeV. The ANCs were then deduced from the juxtaposition of DWBA and CC calculations with the experimental angular distributions and the zero energy astrophysical S-factor for 3 He( α,γ ) 7 Be reaction was calculated to equal 0.534 ± 0.025 keVb. Both our experimental and theoretical approaches were tested through the analysis of the 6 Li(p, γ ) 7 Be astrophysical factor, with further interesting astrophysical implications.

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