TY - JOUR
T1 - Transmutation of 239Pu with spallation neutrons
AU - Wan, J. S.
AU - Langrock, E. J.
AU - Westmeier, W.
AU - Vater, P.
AU - Brandt, R.
AU - Adam, J.
AU - Balabekian, A.
AU - Bamblevski, V. P.
AU - Barabanov, M. Yu
AU - Bradnova, V.
AU - Chaloun, P.
AU - Kalinnikov, V. G.
AU - Krasnov, V. A.
AU - Krivopustov, M. I.
AU - Kulakov, B. A.
AU - Perelygin, V. P.
AU - Pronskikh, V. S.
AU - Solnyshkin, A. A.
AU - Sosnin, A. N.
AU - Stegailov, V. I.
AU - Tsoupko-Sitnikov, V. M.
AU - Modolo, G.
AU - Odoj, R.
AU - Hashemi-Nezhad, S. R.
AU - Zamani-Vallasiadou, M.
PY - 2001
Y1 - 2001
N2 - Incineration studies of plutonium were carried out at the Synchrophasotron of the Joint Institute for Nuclear Research (JINR), Dubna, using proton beams with energies of 0.53 GeV and 1.0 GeV. Solid lead targets (8 cm in diameter and 20 cm long) were surrounded with 6 cm thick paraffin as neutron moderator and then irradiated. The transmutation of 239Pu and the associated production of fission products 91Sr, 92Sr, 97Zr, 99Mo, 103Ru, 105Ru, 129Sb, 132Te, 133I, 135I and 143Ce were studied in the present work. The plutonium samples (each 449 mg) were placed on the outer surface of moderator. For 1.0 GeV proton beam, the fission rate of 239Pu is 0.0032 atoms per proton in one gram plutonium samples, for 0.53 GeV proton, this value is 0.0022. The experimental uncertainty is about 15%. The experiments are compared to two theoretical model calculations with moderate success, using the Dubna Cascade Model (CEM) and the LAHET code. The practical incineration rate of 239Pu is very high. For example: if one uses 10 mA, 1 GeV proton beams under the same (fictive) experimental conditions, the incineration rate of 239Pu via fission is 3 mg out of the 449 mg sample per day. For 0.53 GeV protons the corresponding rate is 2 mg per day.
AB - Incineration studies of plutonium were carried out at the Synchrophasotron of the Joint Institute for Nuclear Research (JINR), Dubna, using proton beams with energies of 0.53 GeV and 1.0 GeV. Solid lead targets (8 cm in diameter and 20 cm long) were surrounded with 6 cm thick paraffin as neutron moderator and then irradiated. The transmutation of 239Pu and the associated production of fission products 91Sr, 92Sr, 97Zr, 99Mo, 103Ru, 105Ru, 129Sb, 132Te, 133I, 135I and 143Ce were studied in the present work. The plutonium samples (each 449 mg) were placed on the outer surface of moderator. For 1.0 GeV proton beam, the fission rate of 239Pu is 0.0032 atoms per proton in one gram plutonium samples, for 0.53 GeV proton, this value is 0.0022. The experimental uncertainty is about 15%. The experiments are compared to two theoretical model calculations with moderate success, using the Dubna Cascade Model (CEM) and the LAHET code. The practical incineration rate of 239Pu is very high. For example: if one uses 10 mA, 1 GeV proton beams under the same (fictive) experimental conditions, the incineration rate of 239Pu via fission is 3 mg out of the 449 mg sample per day. For 0.53 GeV protons the corresponding rate is 2 mg per day.
UR - http://www.scopus.com/inward/record.url?scp=0035112668&partnerID=8YFLogxK
U2 - 10.1023/A:1006787703538
DO - 10.1023/A:1006787703538
M3 - Article
AN - SCOPUS:0035112668
SN - 0236-5731
VL - 247
SP - 151
EP - 157
JO - Journal of Radioanalytical and Nuclear Chemistry
JF - Journal of Radioanalytical and Nuclear Chemistry
IS - 1
ER -