Proton induced fission of 232Th at intermediate energies
- Authors: Gikal K.B.1, Trzaska W.H.2, Sahiev S.K.3, Rubchenya V.A.2,4, Piasecki E.5, Kvochkina T.N.3, Kovalchuk K.V.3, Knyazhev G.N.1, Itkis M.G.1, Itkis I.M.1, Edomskiy A.V.3, Burtebaev N.T.3, Bogachev A.A.1, Kozulin E.M.1, Vardaci E.6
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Affiliations:
- Flerov Laboratory of Nuclear Reactions
- Department of Physics
- Institute of Nuclear Physics of Ministry of Energy of the Republic of Kazakhstan
- V.G. Khlopin Radium Institute
- Heavy Ion Laboratory of Warsaw University
- INFN Napoli, Dipartimento di Scienze Fisiche dell’Università di Napoli
- Issue: Vol 79, No 9-10 (2016)
- Pages: 1367-1374
- Section: Fission Physics
- URL: https://journal-vniispk.ru/1063-7788/article/view/191083
- DOI: https://doi.org/10.1134/S1063778816090040
- ID: 191083
Cite item
Abstract
The mass-energy distributions and cross sections of proton-induced fission of 232Th have been measured at the proton energies of 7, 10, 13, 20, 40, and 55 MeV. Experiments were carried out at the proton beam of the K-130 cyclotron of the JYFL Accelerator Laboratory of the University of Jyväskylä and U-150m cyclotron of the Institute of Nuclear Physics, Ministry of Energy of the Republic of Kazakhstan. The yields of fission fragments in the mass range A = 60–170 a.m.u. have been measured up to the level of 10−4%. The three humped shape of the mass distribution up has been observed at higher proton energies. The contribution of the symmetric component grows up with increasing proton incident energy; although even at 55 MeV of proton energy the shoulders in the mass energy distribution clearly indicate the asymmetric fission peaks. Evolution of shell structure was observed in the fission fragment mass distributions even at high excitation energy.
About the authors
K. B. Gikal
Flerov Laboratory of Nuclear Reactions
Author for correspondence.
Email: kgikal@mail.ru
Russian Federation, Dubna, 141980
W. H. Trzaska
Department of Physics
Email: kgikal@mail.ru
Finland, Jyväskylä, FIN-40351
S. K. Sahiev
Institute of Nuclear Physics of Ministry of Energy of the Republic of Kazakhstan
Email: kgikal@mail.ru
Kazakhstan, Almaty, 050032
V. A. Rubchenya
Department of Physics; V.G. Khlopin Radium Institute
Email: kgikal@mail.ru
Finland, Jyväskylä, FIN-40351; St. Petersburg, 194021
E. Piasecki
Heavy Ion Laboratory of Warsaw University
Email: kgikal@mail.ru
Poland, Warsaw
T. N. Kvochkina
Institute of Nuclear Physics of Ministry of Energy of the Republic of Kazakhstan
Email: kgikal@mail.ru
Kazakhstan, Almaty, 050032
K. V. Kovalchuk
Institute of Nuclear Physics of Ministry of Energy of the Republic of Kazakhstan
Email: kgikal@mail.ru
Kazakhstan, Almaty, 050032
G. N. Knyazhev
Flerov Laboratory of Nuclear Reactions
Email: kgikal@mail.ru
Russian Federation, Dubna, 141980
M. G. Itkis
Flerov Laboratory of Nuclear Reactions
Email: kgikal@mail.ru
Russian Federation, Dubna, 141980
I. M. Itkis
Flerov Laboratory of Nuclear Reactions
Email: kgikal@mail.ru
Russian Federation, Dubna, 141980
A. V. Edomskiy
Institute of Nuclear Physics of Ministry of Energy of the Republic of Kazakhstan
Email: kgikal@mail.ru
Kazakhstan, Almaty, 050032
N. T. Burtebaev
Institute of Nuclear Physics of Ministry of Energy of the Republic of Kazakhstan
Email: kgikal@mail.ru
Kazakhstan, Almaty, 050032
A. A. Bogachev
Flerov Laboratory of Nuclear Reactions
Email: kgikal@mail.ru
Russian Federation, Dubna, 141980
E. M. Kozulin
Flerov Laboratory of Nuclear Reactions
Email: kgikal@mail.ru
Russian Federation, Dubna, 141980
E. Vardaci
INFN Napoli, Dipartimento di Scienze Fisiche dell’Università di Napoli
Email: kgikal@mail.ru
Italy, Napoli
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