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Program - Brookhaven National Laboratory

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and time) of the probability distribution functions that describe the correlated time dependent locations<br />

of the atoms. Previously, significant assumptions were used to allow the calculation of such correlation<br />

functions and subsequently S(α,β) for various atomic systems. More recently, a predictive approach based<br />

on ab initio quantum mechanics or classical molecular dynamics has been formulated to estimate S(α,β).<br />

In principle, these modern atomistic simulation methods make it possible to generate the inelastic thermal<br />

neutron scattering cross sections of any material and to accurately reflect the physical conditions of<br />

the medium (i.e, temperature, pressure, etc.). In addition, the generated cross sections are free from assumptions<br />

such as the incoherent approximation of scattering theory and, in the case of solids, crystalline<br />

perfection. As a result, new and improved thermal neutron scattering data libraries have been generated<br />

for a variety of materials. Among these are reactor moderators and reflectors such as reactor-grade graphite<br />

and beryllium (with coherent inelastic scattering), beryllium carbide, silicon dioxide, cold and ultracold<br />

neutron media such as solid methane and solid deuterium, and neutron beam filters such as sapphire and<br />

bismuth. Consequently, it is anticipated that the above approach will play a major role in providing the<br />

nuclear science and engineering community with its needs of thermal neutron scattering data especially<br />

when considering new materials where experimental information may be scarce or nonexistent.<br />

HC 5 5:00 PM<br />

Level Density Options for Hauser-Feshbach Model Calculations from an Experimental<br />

Point of View<br />

A.V. Voinov, S.M. Grimes, C.R. Brune, T.N. Massey<br />

Department of Physics and Astronomy, Ohio University, Athens Ohio 45701<br />

The current generation of nuclear reaction codes uses many options for level density inputs which affect<br />

cross section calculations to a large extent. Level density parameters determined on the basis of the neutron<br />

resonance data obviously experience problems related to both unknown spin and parity distributions at<br />

neutron resonance energies and way the level density is extrapolated towards the discrete level region.<br />

Therefore, the extensive tests of available input level density options in modern reaction codes are needed.<br />

Particle spectra from compound nuclear reactions are very sensitive to level densities of residual nuclei.<br />

We have measured neutron, proton and alpha spectra from reactions induced by deuterons, 3 He, alpha<br />

particles and 6,7 Li beams from the tandem accelerator of the Edwards <strong>Laboratory</strong>. It is seen that at beam<br />

energies around 2-4 MeV/A spectra measured at backward angles do not significantly depend on the type<br />

of incoming species indicating that the compound reaction mechanism is dominant. Experimental particle<br />

spectra have been compared to calculations from the Empire nuclear reaction code [1] employing different<br />

input options for the level density model. It is shown that calculations are sensitive to input level densities<br />

and it is possible to rule out some of the models. Particularly, we found that for the mass range 50-60,<br />

the level density model must include the constant temperature formula. The model based on Gilbert and<br />

Cameron formulation [2] is the best to describe compound nuclear reactions in this mass range. Empire<br />

calculations against experimental data are presented.<br />

[1] M. Herman, R. Capote, B. Carlson, P. Oblozinsky, M. Sin, A.Trkov, H. Wienke and V. Zerkin, Nucl.<br />

Data Sheets 108, (2007) 2655. [2] A. Gilbert, F. S.Chen and A. G. W. Cameron, Can. J. Phys 43, (1965)<br />

1248.<br />

HC 6 5:15 PM<br />

Cross Section Calculation of Deuteron-Induced Reactions Using Extended CCONE Code<br />

117

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