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Program - Brookhaven National Laboratory

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However, experiments often measure level densities, in which levels are counted without including their<br />

spin degeneracies. A spin projection method [4] enables us to also calculate level densities in SMMC. We<br />

have calculated the level density of 162Dy and found it to agree well with neutron resonance and level<br />

counting data, and with the level density measured by the “Oslo” method [5]. This work was supported<br />

in part by the Department of Energy grant DE-FG-0291-ER-40608.<br />

[1] Y. Alhassid, L. Fang and H. Nakada, Phys. Rev. Lett. 101, 082501 (2008); Journal of Physics:<br />

Conference Series 267, 012033 (2011). [2] C. Özen, Y. Alhassid and H. Nakada, arXiv:1206.6773 (2012).<br />

[3] A. Mukherjee and Y. Alhassid, Phys. Rev. Lett. 109, 032503 (2012). [4] Y. Alhassid, S. Liu and H.<br />

Nakada, Phys. Rev. Lett. 99, 162504 (2007). [5] Y. Alhassid and M. Bonett-Matiz (2012).<br />

PC 4 4:40 PM<br />

The Theoretical Calculation of Actinide Nuclear Reaction Data<br />

Yinlu Han, Yongli Xu, Haiying Liang, Hairui Guo, Qingbiao Shen<br />

China Institute of Atomic Energy, P.O. Box 275(41), Beijing 102413, People’s Republic of China<br />

Chonghai Cai<br />

Department of Physics, Nankai University, Tianjin 300071, People’s Republic of China<br />

Neutron-induced reactions on Actinides in the energy range below 200 MeV are of fundamental importance<br />

in the field of nuclear energy and nuclear transmutation. For example, these interactions dominate neutron<br />

generation and neutron transport in accelerator supported nuclear reactors, such as proposed accelerator<br />

driven systems. Knowledge of accurate neutron-induced fission cross sections is crucially important for the<br />

design of various reactor systems. On the other hand, since neutron, proton, deuteron, triton, and alphaparticle<br />

emission double differential cross sections and spectra provide a complementary information on<br />

prompt fission neutrons and nuclear reaction mechanisms, theoretical model calculation can provide more<br />

information about nucleus structure and nuclear reaction. All cross sections of neutron-induced reactions,<br />

angular distributions, double differential cross sections, angle-integrated spectra, prompt fission neutron<br />

spectra, γ-ray production cross sections and energy spectra are calculated by using theoretical models for<br />

n+ 232 Th, 233,234,235,236,237,238 U, 237 Np, 239,240,241,242 Pu, 241,242,243 Am at incident neutron energies from 0.01<br />

to 200 MeV. The optical model, the unified Hauser-Feshbach and exciton model which included the improved<br />

Iwamoto-Harada model, the fission model, the linear angular momentum dependent exciton density<br />

model, the coupled channel theory, the distorted wave Born approximation and recent experimental data<br />

are used. The present consistent theoretical calculated results are in good agreement with recent experimental<br />

data for incident neutron energy 200 MeV. The evaluated data of neutron induced nuclear reaction<br />

from ENDF/B-VII, JENDL-4.0 are compared with present calculated results and existing experimental<br />

data. The calculated results are given in ENDF/B format.<br />

PC 5 5:00 PM<br />

Cluster Emission for the Pre-Equilibrium Exciton Model with Spin Variables<br />

E. Betak<br />

Institite of Physics SAS, 84511 Bratislava, Slovakia and Fac.Filos.& Sci., Sliesian Univ, 74601 Opava,<br />

Czech Rep.<br />

Angular momentum variables have been added into the pre-equilibrium exciton model by Obloˇzinsk´y and<br />

Chadwick [1] to handle the equilibration process, nucleon- and γ-emissions. The emission of ligth clusters<br />

(complex particles), i.e. deuterons to α’s, remained essentially intact by this effort. Our approach stems<br />

230

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