Phys.Rev. C 89, 035806 (2014)

C.Langer, O.Lepyoshkina, Y.Aksyutina, T.Aumann, S.Beceiro Novo, J.Benlliure, K.Boretzky, M.Chartier, D.Cortina, U.Datta Pramanik, O.Ershova, H.Geissel, R.Gernhauser, M.Heil, G.Ickert, H.T.Johansson, B.Jonson, A.Kelic-Heil, A.Klimkiewicz, J.V.Kratz, R.Krucken, R.Kulessa, K.Larsson, T.Le Bleis, R.Lemmon, K.Mahata, J.Marganiec, T.Nilsson, V.Panin, R.Plag, W.Prokopowicz, R.Reifarth, V.Ricciardi, D.M.Rossi, S.Schwertel, H.Simon, K.Summerer, B.Streicher, J.Taylor, J.R.Vignote, F.Wamers, C.Wimmer, P.Z.Wu

Thermonuclear reaction ³⁰S(p, γ)³¹Cl studied via Coulomb breakup of ³¹Cl

NUCLEAR REACTIONS Pb(³¹Cl, p), [³¹Cl secondary beam from ⁹Be(³⁶Ar, X), E=825 MeV/nucleon primary reaction], E=650 MeV/nucleon; measured reaction products, fragment spectra, Eγ, Iγ at R³B-LAND-GSI facility. ³¹Cl; deduced levels, resonances, J, π, width, comparison with levels predicted in shell-model calculations. ³⁰S(p, γ), T=0.08-2.00 GK; deduced thermonuclear reaction rates. Relevance to rp process in typical Type I x-ray burst conditions.

doi: 10.1103/PhysRevC.89.035806