Properties of Na20, Al24, P28, Cl32, and K36 for studies of explosive hydrogen burning

C. Wrede, J. A. Clark, C. M. Deibel, T. Faestermann, R. Hertenberger, A. Parikh, H.-F. Wirth, S. Bishop, A. A. Chen, K. Eppinger, B. M. Freeman, R. Krücken, O. Lepyoshkina, G. Rugel, and K. Setoodehnia
Phys. Rev. C 82, 035805 – Published 29 September 2010

Abstract

The radiative proton-capture reactions Ne19(p,γ)Na20, Mg23(p,γ)Al24, Si27(p,γ)P28, S31(p,γ)Cl32, and Ar35(p,γ)K36 potentially influence energy generation and/or nucleosynthesis during explosive hydrogen burning in classical novae and/or type I x-ray bursts. The thermonuclear rates of these reactions are dependent on resonance energies Er=ExQ and strengths ωγ. The Ne20(He3,t)Na20, Mg24(He3,t)Al24, Si28(He3,t)P28, S32(He3,t)Cl32, and Ar36(He3,t)K36 reactions have been measured using a 32-MeV, He32+ beam; ion-implanted carbon-foil targets developed at the University of Washington; and the Munich Q3D magnetic spectrograph. This experiment has already yielded precision mass measurements of Na20, Al24, P28, and Cl32 [C. Wrede et al., Phys. Rev. C 81, 055503 (2010)], which are used presently to constrain the corresponding (p,γ) reaction Q values. The new Al24 and P28 masses resolve a discrepancy in the energy of the lowest-energy resonance in the Mg23(p,γ)Al24 reaction and better constrain a direct measurement of its strength. Excitation energies in Cl32 and K36 have also been measured. An important new proton-unbound level has been found at Ex=2196.9(7) keV in K36 and the uncertainties in K36 excitation energies have been reduced by over an order of magnitude. Using the new data on K36, the A=36, T=1 triplets have been reassigned. The thermonuclear Ar35(p,γ)K36 reaction rate is found to be much higher than a commonly adopted rate and this could affect energy generation in type I x-ray bursts.

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  • Received 10 August 2010

DOI:https://doi.org/10.1103/PhysRevC.82.035805

©2010 American Physical Society

Authors & Affiliations

C. Wrede1,2, J. A. Clark2,3, C. M. Deibel2,3,4, T. Faestermann5, R. Hertenberger6, A. Parikh5, H.-F. Wirth6, S. Bishop5, A. A. Chen7,8, K. Eppinger5, B. M. Freeman1, R. Krücken5, O. Lepyoshkina5, G. Rugel5, and K. Setoodehnia7

  • 1Department of Physics, University of Washington, Seattle, Washington 98195, USA
  • 2Wright Nuclear Structure Laboratory, Yale University, New Haven, Connecticut 06520, USA
  • 3Physics Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 4Joint Institute for Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824, USA
  • 5Physik Department E12, Technische Universität München, D-85748 Garching, Germany
  • 6Fakultät für Physik, Ludwigs-Maximilians-Universität München, D-85784 Garching, Germany
  • 7Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada
  • 8DFG Cluster of Excellence Origin and Structure of the Universe, Technische Universität München, D-85748 Garching, Germany

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Vol. 82, Iss. 3 — September 2010

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