Program - Brookhaven National Laboratory
Program - Brookhaven National Laboratory
Program - Brookhaven National Laboratory
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in inverse kinematics. I will present the measurement of (γ, n) reactions at the LAND/R3B setup at GSI<br />
Darmstadt, focussing on the recent development of the high resolution fast neutron detector NeuLAND.<br />
This detection system will allow measurements of the (γ, n) channel with unprecedented accuracy and<br />
thus provide important information about neutron capture cross section on radioactive species in the<br />
astrophysically interesting energy regime.<br />
PR 5<br />
Nuclear Data Processing and Dissemination Efforts for Nuclear Astrophysics at ORNL<br />
Caroline D. Nesaraja, Michael S. Smith, Physics Division, Oak Ridge <strong>National</strong> <strong>Laboratory</strong>, Oak Ridge,<br />
Tennessee, 37831. USA. Eric J. Lingerfelt, Computer Science and Mathematics Division, Oak Ridge<br />
<strong>National</strong> <strong>Laboratory</strong>, Oak Ridge, Tennessee, 37831. USA.<br />
At research facilities around the world, nuclear astrophysics measurements are being made with radioactive<br />
and stable beams to enhance our understanding of the evolution and explosion of stars and their creation<br />
of elements. For these extensive data to be effectively used in astrophysical simulations, they must be<br />
evaluated, processed, and disseminated to the community. As the amount of data acquired in this field increases,<br />
there have been efforts to streamline these processes. One example is an online software system, the<br />
Computational Infrastructure for Nuclear Astrophysics (CINA). Utilized by researchers in 126 institutions<br />
and 29 countries, CINA can generate thermonuclear reaction rates from nuclear data input, incorporate<br />
rates into libraries, and run and visualize astrophysics simulations with these libraries. CINA, freely available<br />
online at nucastrodata.org, consists of a suite of codes which provide data processing, management,<br />
visualization, and dissemination capabilities, as well as workflow management. We will describe some of<br />
these features of CINA with examples of reaction rate calculations, simulations, and disseminations.<br />
PR 6<br />
Low Level Densities of Exotic 131,133 Sn Isotopes and Impact on r-process Nucleosynthesis<br />
Shi-Sheng Zhang, School of Physics and Nuclear Energy Engineering, Beihang Univ., Beijing, China.<br />
M.S. Smith, Physics Division, Oak Ridge <strong>National</strong> <strong>Laboratory</strong>, Oak Ridge, TN, USA. G. Arbanas,<br />
Reactor and Nuclear Systems Division, Oak Ridge <strong>National</strong> <strong>Laboratory</strong>, Oak Ridge, TN, USA. R.L.<br />
Kozub, Dept. of Physics, Tennessee Technological Univ., Cookeville, TN, USA.<br />
Neutron capture rates on unstable nuclei near the doubly-magic exotic 132 Sn were recently shown to<br />
significantly impact the synthesis of heavy elements in the r-process in supernovae [1]. These rates are<br />
usually determined from cross sections estimated with statistical models employing a Fermi gas level<br />
density formulation. Such an approach is only valid if the density of levels in the compound nucleus is<br />
sufficiently high. We examine the validity of this assumption for neutron capture on 130,132 Sn by making<br />
self-consistent calculations of single-particle bound and resonant levels in 131,133 Sn using the analytical<br />
continuation of the coupling constant (ACCC) based on a relativistic mean field (RMF) theory with BCS<br />
approximation. Knowledge of bound states with a strong single particle nature can be used to calculate<br />
direct neutron capture, and information on single particle resonances above the neutron capture threshold<br />
can be used to determine the level density for statistical models – as well as to calculate capture into<br />
individual resonances. Our RMF+ACC+BCS model predicts four strong single-particle bound levels in<br />
both 131,133 Sn with an ordering that agrees with recent transfer reaction experiments [2,3] and spacings<br />
that, while differing from experiment, are consistent between the Sn isotopes. In 131 Sn and 133 Sn, we also<br />
find at most one single-particle level in the effective energy range for neutron captures in the r-process<br />
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