/ Experiment-Nucl

Secondary particle distributions in an extended uranium target under irradiation by proton, deuteron, and carbon beams

Adam, J. (Prague, Inst. Phys.) ; Baldin, A.A. (Dubna, JINR) ; Baznat, M. (IAP, Chisinau) ; Berlev, A.I. (Dubna, JINR) ; Gusak, K.V. (Joint Inst. Power Nucl. Res., Minsk) ; Kudashkin, I.V. (Dubna, JINR) ; Khushvaktov, J. (Dubna, JINR) ; Paraipan, M. (Bucharest, Inst. Space Science) ; Pronskikh, V.S. (Fermilab) ; Solnyshkin, A.A. (Dubna, JINR) ; Sotnikov, V. (Kharkov, KIPT) ; Stegaylov, V.I. (Dubna, JINR) ; Tyutyunikov, S.I. (Dubna, JINR) ; Voronko, V. (Kharkov, KIPT) ; Zeman, M. (Masaryk U., Brno) ; Zhuk, I. (Joint Inst. Power Nucl. Res., Minsk)

Published in: Nucl.Instrum.Meth.
Year: 2017
Vol.: A872
Page No: 87-92
Year: 2017-08-12

Abstract: The spatial distribution of particle fluences in the extended uranium target (“Quinta” assembly) irradiated by 0.66 GeV proton, 4 AGeV deuteron and carbon beams is studied by analyzing the accumulation rates of the isotopes with different threshold energy (E) in Co samples. The accumulation rates for the following isotopes: Co (E 0 MeV), Fe (E 3 MeV), Co (E 10 MeV), Co (E 20 MeV), Co (E 32 MeV), Sc (E 55 MeV) , and V (E 70 MeV) were measured using the HPGe spectrometer. The experimental accumulation rates and the reconstructed neutron spectra are compared with the simulations using the codes Geant4 and MARS15. The noticeable difference between the simulated and the experimental data, especially in the hard part of the neutron spectrum, is analyzed.

Total numbers of views: 140
Numbers of unique views: 66
DOI: 10.1016/j.nima.2017.08.009
 Record created 2017-11-02, last modified 2017-11-02

Rate this document:

Rate this document:
(Not yet reviewed)