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rp-process nucleosynthesis at extreme temperature and density conditions

H. SchatzUniversity of Notre Dame, Dept. of Physics, Notre Dame, IN 46556, USAA. AprahamianUniversity of Notre Dame, Dept. of Physics, Notre Dame, IN 46556, USAJ. GörresUniversity of Notre Dame, Dept. of Physics, Notre Dame, IN 46556, USAM. WiescherUniversity of Notre Dame, Dept. of Physics, Notre Dame, IN 46556, USAT. RauscherUniversität Basel, Institut für theoretische Physik, CH-4056 Basel, SwitzerlandJ.F. RembgesUniversität Basel, Institut für theoretische Physik, CH-4056 Basel, SwitzerlandF.‐K. ThielemannUniversität Basel, Institut für theoretische Physik, CH-4056 Basel, SwitzerlandB. PfeifferUniversität Mainz, Institut für Kernchemie, D-55099 Mainz, GermanyP. MöllerUniversität Mainz, Institut für Kernchemie, D-55099 Mainz, GermanyKarl KratzUniversität Mainz, Institut für Kernchemie, D-55099 Mainz, GermanyH. HerndlTechnische Universität Wien, Institut für Kernphysik, A-1040 Wien, AustriaB. A. BrownMichigan State University, Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, East Lansing, MI 48824, USAH. RebelForschungszentrum Karlsruhe, Institut für Kernphysik III, D-76021 Karlsruhe, Germany
1998en
ABI

Аннотация

We present nuclear reaction network calculations to investigate the influence of nuclear structure on the rp-process between Ge and Sn in various scenarios. Due to the lack of experimental data for neutron-deficient nuclei in this region, we discuss currently available model predictions for nuclear masses and deformations as well as methods of calculating reaction rates (Hauser-Feshbach) and β-decay rates (QRPA and shell model). In addition, we apply a valence nucleon (NpNn) correlation scheme for the prediction of masses and deformations. We also describe the calculations of 2p-capture reactions, which had not been considered before in this mass region. We find that in X-ray bursts 2p-capture reactions accelerate the reaction flow into the Z ≥ 36 region considerably. Therefore, the rp-process in most X-ray bursts does not end in the Z = 32–36 region as previously assumed and overproduction factors of 107–108 are reached for some light p-nuclei in the A = 80–100 region. This might be of interest in respect of the yet unexplained large observed solar system abundances of these nuclei. Nuclei in this region can also be produced via the rp-proces in accretion disks around low mass black holes. Our results indicate that the rp-process energy production in the Z > 32 region cannot be neglected in these scenarios. We discuss in detail the influence of the various nuclear structure input parameters and their current uncertainties on these results. It turns out that rp-process nucleosynthesis is mainly determined by nuclear masses and β-decay rates of nuclei along the proton drip line. We present a detailed list of nuclei for which mass or β-decay rate measurements would be crucial to further constrain the models.

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