Search

Your search keyword '"Edomskiy, A."' showing total 3 results
Start Over Author "Edomskiy, A."
3 results on '"Edomskiy, A."'

2. Proton induced fission of 232Th at intermediate energies

Author

E. Piasecki, K. B. Gikal, G. N. Knyazhev, S. K. Sahiev, K. V. Kovalchuk, N. T. Burtebaev, M. G. Itkis, Emanuele Vardaci, A. V. Edomskiy, I. M. Itkis, T. N. Kvochkina, E. M. Kozulin, Wladyslaw Henryk Trzaska, V. A. Rubchenya, A. A. Bogachev, Gikal, K. B., Kozulin, E. M., Bogachev, A. A., Burtebaev, N. T., Edomskiy, A. V., Itkis, I. M., Itkis, M. G., Knyazhev, G. N., Kovalchuk, K. V., Kvochkina, T. N., Piasecki, E., Rubchenya, V. A., Sahiev, S. K., Trzaska, W. H., and Vardaci, Emanuele

Subjects
Nuclear and High Energy Physics, Cold fission, fission dynamics, Proton, Fission, Nuclear Theory, Cyclotron, 01 natural sciences, law.invention, Nuclear physics, induced fission, law, 0103 physical sciences, Proton emission, Nuclear Experiment, 010306 general physics, Physics, Range (particle radiation), Cluster decay, Mass distribution, ta114, 010308 nuclear & particles physics, mass-energy distributions, Atomic and Molecular Physics, and Optics, proton and neutron, Physics::Accelerator Physics, Atomic physics
Abstract

The mass-energy distributions and cross sections of proton-induced fission of Th-232 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 Jyvakyla 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.

Published
2016

3. Proton induced fission of Th at intermediate energies.

Author

Gikal, K., Kozulin, E., Bogachev, A., Burtebaev, N., Edomskiy, A., Itkis, I., Itkis, M., Knyazhev, G., Kovalchuk, K., Kvochkina, T., Piasecki, E., Rubchenya, V., Sahiev, S., Trzaska, W., and Vardaci, E.

Subjects
NUCLEAR fission, PROTONS, NUCLEAR cross sections, CYCLOTRONS, MASS (Physics), NUCLEAR excitation
Abstract

The mass-energy distributions and cross sections of proton-induced fission of Th 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. [ABSTRACT FROM AUTHOR]

Published
2016
Full Text
View/download PDF

Catalog

Books, media, physical & digital resources
See catalog results