Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction

The 12C(α, γ)16O reaction plays a key role in the evolution of stars with masses of M > 0.55 M⊙. At the Gamow peak (Ec.m. = 300 ke V, T9 = 0.2), the cross section of the 12C(α, γ)16O reaction is so small (about 10−17 barn) that the direct measurement in ground laboratory is not feasible with the...

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Main Authors: Guo B., Du X.C., Li Z.H., Li Y.J., Pang D.Y., Su J., Yan S.Q., Fan Q.W., Gan L., Han Z.Y., Li E.T., Li X.Y., Lian G., Liu J.C., Pei C.J., Qiao L.H., Shen Y.P., Su Y., Wang Y.B., Zeng S., Zhou Y., Liu W.P.
Format: Article
Language:English
Published: EDP Sciences 2016-01-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/201610904003
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spelling doaj-4660e31ebfbc40f8a1da1bfea91d32f02021-08-02T11:07:47ZengEDP SciencesEPJ Web of Conferences2100-014X2016-01-011090400310.1051/epjconf/201610904003epjconf_omeg2016_04003Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reactionGuo B.0Du X.C.1Li Z.H.2Li Y.J.3Pang D.Y.Su J.4Yan S.Q.5Fan Q.W.6Gan L.7Han Z.Y.8Li E.T.9Li X.Y.10Lian G.11Liu J.C.12Pei C.J.13Qiao L.H.14Shen Y.P.15Su Y.16Wang Y.B.17Zeng S.18Zhou Y.19Liu W.P.20China Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyCollege of Physics Science and Technology, Shenzhen UniversityChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyChina Institute of Atomic EnergyThe 12C(α, γ)16O reaction plays a key role in the evolution of stars with masses of M > 0.55 M⊙. At the Gamow peak (Ec.m. = 300 ke V, T9 = 0.2), the cross section of the 12C(α, γ)16O reaction is so small (about 10−17 barn) that the direct measurement in ground laboratory is not feasible with the existing technology. Up to now, the cross sections at lower energies can only be extrapolated from the data at higher energies. However, two subthreshold resonances, locating at Ex = 7.117 MeV and Ex = 6.917 MeV, make this extrapolation more complicated. In this work the 6.917 MeV subthreshold resonance in the 12C(α, γ)16O reaction was investigated via the 12C(11B, 7Li)16O reaction. The experiment was performed using the Q3D magnetic spectrograph at HI-13 tandem accelerator. We measured the angular distribution of the 12C(11B, 7Li)16O transfer reaction leading to the 6.917 MeV state. Based on DWBA analysis, we derived the square of ANC of the 6.917 MeV level in 16O to be (2.45± 0.28) ×1010 fm−1, with which the reduced-α width can be computed. Finally, we calculated the astrophysical SE2 factor of the 6.917 MeV resonance to be 67.6 ± 7.7 ke V b.http://dx.doi.org/10.1051/epjconf/201610904003
collection DOAJ
language English
format Article
sources DOAJ
author Guo B.
Du X.C.
Li Z.H.
Li Y.J.
Pang D.Y.
Su J.
Yan S.Q.
Fan Q.W.
Gan L.
Han Z.Y.
Li E.T.
Li X.Y.
Lian G.
Liu J.C.
Pei C.J.
Qiao L.H.
Shen Y.P.
Su Y.
Wang Y.B.
Zeng S.
Zhou Y.
Liu W.P.
spellingShingle Guo B.
Du X.C.
Li Z.H.
Li Y.J.
Pang D.Y.
Su J.
Yan S.Q.
Fan Q.W.
Gan L.
Han Z.Y.
Li E.T.
Li X.Y.
Lian G.
Liu J.C.
Pei C.J.
Qiao L.H.
Shen Y.P.
Su Y.
Wang Y.B.
Zeng S.
Zhou Y.
Liu W.P.
Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction
EPJ Web of Conferences
author_facet Guo B.
Du X.C.
Li Z.H.
Li Y.J.
Pang D.Y.
Su J.
Yan S.Q.
Fan Q.W.
Gan L.
Han Z.Y.
Li E.T.
Li X.Y.
Lian G.
Liu J.C.
Pei C.J.
Qiao L.H.
Shen Y.P.
Su Y.
Wang Y.B.
Zeng S.
Zhou Y.
Liu W.P.
author_sort Guo B.
title Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction
title_short Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction
title_full Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction
title_fullStr Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction
title_full_unstemmed Astrophysical SE2 factor of the 12C(α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction
title_sort astrophysical se2 factor of the 12c(α, γ)16o reaction through the 12c(11b, 7li)16o transfer reaction
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2016-01-01
description The 12C(α, γ)16O reaction plays a key role in the evolution of stars with masses of M > 0.55 M⊙. At the Gamow peak (Ec.m. = 300 ke V, T9 = 0.2), the cross section of the 12C(α, γ)16O reaction is so small (about 10−17 barn) that the direct measurement in ground laboratory is not feasible with the existing technology. Up to now, the cross sections at lower energies can only be extrapolated from the data at higher energies. However, two subthreshold resonances, locating at Ex = 7.117 MeV and Ex = 6.917 MeV, make this extrapolation more complicated. In this work the 6.917 MeV subthreshold resonance in the 12C(α, γ)16O reaction was investigated via the 12C(11B, 7Li)16O reaction. The experiment was performed using the Q3D magnetic spectrograph at HI-13 tandem accelerator. We measured the angular distribution of the 12C(11B, 7Li)16O transfer reaction leading to the 6.917 MeV state. Based on DWBA analysis, we derived the square of ANC of the 6.917 MeV level in 16O to be (2.45± 0.28) ×1010 fm−1, with which the reduced-α width can be computed. Finally, we calculated the astrophysical SE2 factor of the 6.917 MeV resonance to be 67.6 ± 7.7 ke V b.
url http://dx.doi.org/10.1051/epjconf/201610904003
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