B. Mei,
T. Aumann,
S. Bishop,
K. Blaum,
K. Boretzky,
F. Bosch,
C. Brandau,
H. Bräuning,
T. Davinson,
I. Dillmann,
C. Dimopoulou,
O. Ershova,
Z. Fülöp,
H. Geissel,
J. Glorius,
G. Gyürky,
M. Heil,
F. Käppeler,
A. Kelic-Heil,
C. Kozhuharov,
C. Langer,
T. Le Bleis,
Y. Litvinov,
G. Lotay,
J. Marganiec,
G. Münzenberg,
F. Nolden,
N. Petridis,
R. Plag,
U. Popp,
G. Rastrepina,
R. Reifarth,
B. Riese,
C. Rigollet,
C. Scheidenberger,
H. Simon,
K. Sonnabend,
M. Steck,
T. Stöhlker,
T. Szücs,
K. Sümmerer,
G. Weber,
H. Weick,
D. Winters,
N. Winters,
P. Woods,
and Q. Zhong
First measurement of the ⁹⁶Ru(p,γ)⁹⁷Rh cross section for the p process with a storage ring
Phys. Rev. C, 92 :035803 (September 2015)
First measurement of the ⁹⁶Ru(p,γ)⁹⁷Rh cross section for the p process with a storage ring
Phys. Rev. C, 92 :035803 (September 2015)
Abstract:
This work presents a direct measurement of the ⁹⁶Ru(p,γ)⁹⁷Rh cross section via a novel technique using a storage ring, which opens opportunities for reaction measurements on unstable nuclei. A proof-of-principle experiment was performed at the storage ring ESR at GSI in Darmstadt, where circulating ⁹⁶Ru ions interacted repeatedly with a hydrogen target. The ⁹⁶Ru(p,γ)⁹⁷Rh cross section between 9 and 11 MeV has been determined using two independent normalization methods. As key ingredients in Hauser-Feshbach calculations, the γ-ray strength function as well as the level density model can be pinned down with the measured (p,γ) cross section. Furthermore, the proton optical potential can be optimized after the uncertainties from the γ-ray strength function and the level density have been removed. As a result, a constrained ⁹⁶Ru(p,γ)⁹⁷Rh reaction rate over a wide temperature range is recommended for p-process network calculations.