Fragment-mass distributions in neutron-induced fission of 232Th and 238U at 33, 45, and 60 MeV
Creators
- Ryzhov, I. V.1, 2, 3, 4, 5
- Yavshits, S. G.1, 2, 3, 4, 5
- Tutin, G. A.1, 2, 3, 4, 5
- Kovalev, N. V.1, 2, 3, 4, 5
- Saulski, A. V.1, 2, 3, 4, 5
- Kudryashev, N. A.1, 2, 3, 4, 5
- Onegin, M. S.1, 2, 3, 4, 5
- Vaishnene, L. A.1, 2, 3, 4, 5
- Gavrikov, Yu. A.1, 2, 3, 4, 5
- Grudzevich, O. T.1, 2, 3, 4, 5
- Simutkin, V. D.1, 2, 3, 4, 5
- Pomp, S.1, 2, 3, 4, 5
- Blomgren, J.1, 2, 3, 4, 5
- Oesterlund, M.1, 2, 3, 4, 5
- Andersson, P.1, 2, 3, 4, 5
- Bevilacqua, R.1, 2, 3, 4, 5
- Meulders, J. P.1, 2, 3, 4, 5
- Prieels, R.1, 2, 3, 4, 5
- 1. Institute of Nuclear Physics, Universite Catholique de Louvain, B-1348 Louvain-la Neuve (Belgium)
- 2. Department of Physics and Astronomy, Uppsala University, Box 516, SE-751 20 Uppsala (Sweden)
- 3. State Technical University, Studgorodok 1, 249020, Kaluga region, Obninsk (Russian Federation)
- 4. Petersburg Nuclear Physics Insitute, 188300, Gatchina, Leningrad district (Russian Federation)
- 5. V. G. Khlopin Radium Institute, Second Murinskiy prospect 28, 194021, Saint Petersburg (Russian Federation)
Description
We have measured fission fragment-mass yields for neutron-induced fission of 232Th and 238U at energies 32.8, 45.3, and 59.9 MeV. The experiments were done at quasimonoenergetic neutron beams of the Cyclotron Research Center at Louvain-la-Neuve. To detect the fission fragments, a multisection Frisch-gridded ionization chamber was used. The measurement and data analysis techniques are discussed in detail. The obtained mass yields are compared to model calculations with the intermediate-energy nuclear reaction code MCFX. The MCFX code is used to calculate the fraction of fissioning nuclei after cascade, preequilibrium, and statistical reaction stages. The formation of mass distributions is considered as a result of oscillations of the mass-asymmetry degree of freedom in the potential well calculated with the temperature-dependent shell correction method. The experimental results as well as the results of the model calculations demonstrate that the probability of symmetric fission increases with incident neutron energy for both nuclei. The comparison also shows that the symmetric fission is more enhanced for thorium than for uranium with increasing neutron energy. We also compare 238U results with available experimental data; the 232Th data were measured for the first time.
Additional details
Identifiers
Publishing Information
- Journal Title
- Physical Review. C, Nuclear Physics
- Journal Volume
- 83
- Journal Issue
- 5
- Journal Page Range
- p. 054603-054603.12
- ISSN
- 0556-2813
- CODEN
- PRVCAN
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 42094287
- Subject category
- S73: NUCLEAR PHYSICS AND RADIATION PHYSICS;
- Descriptors DEI
- ASYMMETRY; COMPARATIVE EVALUATIONS; CORRECTIONS; CYCLOTRONS; DATA ANALYSIS; DEGREES OF FREEDOM; FISSION FRAGMENTS; IONIZATION CHAMBERS; MASS; MASS DISTRIBUTION; MEV RANGE 10-100; NEUTRON BEAMS; NEUTRON REACTIONS; OSCILLATIONS; PROBABILITY; SYMMETRY; TEMPERATURE DEPENDENCE; THORIUM 232 TARGET; URANIUM 238 TARGET
- Descriptors DEC
- ACCELERATORS; BARYON REACTIONS; BEAMS; CYCLIC ACCELERATORS; DISTRIBUTION; ENERGY RANGE; EVALUATION; HADRON REACTIONS; MEASURING INSTRUMENTS; MEV RANGE; NUCLEAR FRAGMENTS; NUCLEAR REACTIONS; NUCLEON BEAMS; NUCLEON REACTIONS; PARTICLE BEAMS; RADIATION DETECTORS; SPATIAL DISTRIBUTION; TARGETS
Optional Information
- Notes
- (c) 2011 American Institute of Physics