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Program - Brookhaven National Laboratory

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Activation Cross Sections of Deuteron Induced Nuclear Reactions on Natural Titanium up<br />

to 24 MeV<br />

Mayeen Uddin Khandaker, Hasan Abu Kassim<br />

Department of Physics, University of Malaya, 50603 Kuala Lumpur, Malaysia<br />

Hiromitsu Haba, Jumpei Kanaya<br />

Nishina Center for Accelerator-Based Science, RIKEN, Wako, Saitama, 351-0198, Japan.<br />

Naohiko Otuka<br />

Nuclear Data Section, Division of Physical and Chemical Sciences, Department of Nuclear Sciences and<br />

Applications, International Atomic Energy Agency, A-1400 Vienna, Austria<br />

Activation cross-sections of the natTi(d,x)43,44m,44g,46,47,48Sc,48V nuclear processes were measured up<br />

to 24 MeV energy by using a stacked-foil activation technique in combination with HPGe γ-ray spectrometry<br />

using the AVF cyclotron of the RIKEN Wako Institute, Japan. The present data were compared<br />

with the theoretical calculations based on the TALYS and the Empire codes, and found only a partial<br />

agreement among them. The thick target integral yields, i.e., induced radioactivity per unit fluence of<br />

24 MeV deuteron were also deduced from the measured cross-sections of the investigated radionuclides.<br />

Note that, natTi(d,x)48V cross sections find significance in monitoring of deuteron beam from thershold<br />

to 50 MeV. The present experimental results will play an important role in enrichment of the literature<br />

data base for deuteron-induced reactions on natural titanium leading to various applications.<br />

PB 8 5:45 PM<br />

Double Differential Cross Sections for Light-Ion Production from C, O, Si, Fe and Bi<br />

Induced by 175 MeV Quasi-Monoenergetic Neutrons<br />

R. Bevilacqua, S. Pomp, C. Gustavsson, M. Osterlund, V. Simutkin, Department of Physics and<br />

Astronomy, Uppsala University, P.O. Box 516, Uppsala, 75120 Sweden. M. Hayashi, S. Hirayama,<br />

Y. Naitou, Y. Watanabe, Department of Advanced Energy Engineering Science, Kyushu University,<br />

Kasuga, Fukuoka 816-8580, Japan. A. Hjalmarsson, A. Prokofiev, The Svedberg <strong>Laboratory</strong>, Uppsala<br />

University, P.O. Box 533, Uppsala, 75121 Sweden. U. Tippawan, Plasma and Beam Physics Research<br />

Facility, Chiang Mai University, P.O. Box 217, Chiang Mai, 50200 Thailand. F.-R. Lecolley, N. Marie,<br />

LPC, ENSICAEN, Universite de Caen, CAEN Cedex, 14050 France. S. Leray, J.-C. David, CEA, Centre<br />

de Saclay, IRFU/Service de Physique Nucleaire, Gif-sur-Yvette, 91191 France. S.G. Mashnik, XCP<br />

Division, Los Alamos <strong>National</strong> <strong>Laboratory</strong>, Los Alamos, New Mexico 87545, USA.<br />

Accelerator-driven incineration of nuclear waste may play an important role in future scenarios both<br />

in countries investing in the nuclear renaissance and in countries deciding to phase out nuclear energy.<br />

However, development of accelerator-driven systems requires new and more reliable neutron-induced crosssection<br />

data in the intermediate region from 20 to 200 MeV. In this energy region the entire structural<br />

properties of the target nucleus may participate in the nuclear reaction, and the nuclear data community<br />

expressed the need to obtain benchmark experimental data to improve present models and evaluated<br />

nuclear data libraries [1]. A series of neutron induced cross-section measurements at 96 MeV have been<br />

conducted at the The Svedberg <strong>Laboratory</strong> (TSL), Uppsala [2]. However, experimental data are still<br />

scarce above 100 MeV. In this perspective, we have measured cross-sections for light-ion production in<br />

the interaction of 175 MeV quasi-monoenergetic neutrons with C, O, Si, Fe and Bi. Measurements were<br />

conducted at TSL using the Medley spectrometer [3]. We will present inclusive double-differential crosssections<br />

for production of protons, deuterons, tritons, 3 He and α-particles, at eight angles in the laboratory<br />

system, from 20 deg to 160 deg. Experimental data are compared with model calculations obtained with<br />

INCL4.5-Abla07, TALYS, a modified version of JQMD [4], and MCNP6. All models are able to reproduce<br />

227

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