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Program - Brookhaven National Laboratory

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egions: the resolved resonances range and the continuum part. The resonance range has been extended<br />

up to 2 MeV (previously 350 keV) and converted in the Reich-Moore R-Matrix approximation. Larson’s<br />

total cross-section and the recent high-resolution inelastic cross-section measurements from IRMM were<br />

used during the data assimilation. For the continuum region, a simultaneous analysis of different reaction<br />

measurements (total, inelastic, charged particle, capture) has been performed with the ECIS/TALYS<br />

codes, interfaced with CONRAD, and an overall good agreement has been achieved. The covariances<br />

data have been produced with a Monte-Carlo marginalization procedure which consists in propagating all<br />

experimental systematic uncertainties to the nuclear reaction model parameters. This 23 Na evaluation has<br />

been successfully processed and tested on several neutronic benchmarks. It will be proposed for the future<br />

JEFF-3.2 library.<br />

Session OC Nuclear Astrophysics<br />

Thursday March 7, 2013<br />

Room: Empire East at 1:30 PM<br />

OC 1 1:30 PM<br />

Wanted! Nuclear Data for Dark Matter Astrophysics<br />

Paolo Gondolo<br />

University of Utah<br />

The nature of cold dark matter is one of the big unsolved questions in physics. A wide spectrum of astronomical<br />

observations from small galaxies to the largest scales can be consistently explained by the presence<br />

of dark matter, in an amount equal on average to about five times the mass in ordinary matter. It is empirically<br />

known that no known particle can be cold dark matter, and many theories exist for dark matter<br />

as a new elementary particle. Numerous searches for dark matter particles are under way: from production<br />

of new candidates in high-energy accelerators, to direct detection of dark matter-nucleus scattering<br />

in underground observatories, to indirect detection of dark matter signals in cosmic rays, gamma rays, or<br />

stars. Direct and indirect dark matter searches rely on observing an excess of events above background,<br />

and a lot of controversies have arisen over the origin of measured excesses (dark matter signal or misconstrued<br />

background?). In my talk I will show that nuclear physics data have become important for dark<br />

matter searches. With the new high-quality cosmic ray measurements from the AMS-02 experiment, the<br />

major uncertainty in modeling cosmic ray fluxes is in the nuclear physics cross sections for spallation and<br />

fragmentation of cosmic rays off interstellar hydrogen and helium. The understanding of direct detection<br />

backgrounds is limited by poor knowledge of cosmic ray activation in detector materials, with order of<br />

magnitude differences between simulation codes. A scarcity of data on nuclear structure functions, especially<br />

spin structure functions, blurs the connection between dark matter theory and experiments. What<br />

is needed, ideally, are new measurements using polarized beams against nuclear targets to furnish spin<br />

structure data, and proton beams and perhaps helium beams against isotopes of He, Li, Be, B, C, N, O,<br />

Fe, Ni (for indirect searches) and Ge, Xe, Ar (for direct searches).<br />

OC 2 2:00 PM<br />

Experimental Studies of the 13,14 B(n, γ) Rates for Nucleosynthesis Towards the r process<br />

S.G. Altstadt, K. Goebel, T. Heftrich, R. Plag, R. Reifarth, Institute for Applied Physics, University of<br />

Frankfurt, Germany. M. Heil, M. Heine, M. Holl, D. Rossi, GSI Helmholtzzentrum fuer<br />

208

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