Fission barriers and other characteristics of nuclei from the uranium region
- Authors: Tolokonnikov S.V.1,2, Borzov I.N.1,3, Lutostansky Y.S.1, Panov I.V.1,4, Saperstein E.E.1,5
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Affiliations:
- National Research Center Kurchatov Institute
- Moscow Institute of Physics and Technology (State University)
- Joint Institute for Nuclear Research
- Institute for Theoretical and Experimental Physics
- National Research Nuclear University MEPhI
- Issue: Vol 80, No 4 (2017)
- Pages: 631-645
- Section: Nuclei
- URL: https://journal-vniispk.ru/1063-7788/article/view/192104
- DOI: https://doi.org/10.1134/S1063778817040275
- ID: 192104
Cite item
Abstract
Fission barriers in nuclei belonging to the uranium region and their other characteristics are calculated on the basis of the FaNDF0 energy density functional. In particular, the neutron-separation energies Sn and S2n, the proton-separation energies Sp, and the beta-transition energiesQβ are calculated for uranium, neptunium, and plutonium isotopes. In addition, the deformation energies and parameters of these nuclei are presented along with their radii. A comparison with the predictions of the Skyrme–Hartree–Fock method implemented with several versions of the Skyrme energy density functionals is performed. The role of the octupole deformation β3 is studied for the 238U nucleus. It is shown that this deformation does not have any significant effect on the first-barrier height B(1)f or ground-state properties. At the same time, the second-barrier height B(2) f decreases by a factor of about two upon taking into account β3. A phase transition at A ~ 260 is found for the three isotopic chains being considered: this point is a bifurcation point at which B(1)f (A) forks into two curves. Of these, the curve B(2)f (A) splits from it, prolonging the former curve for B(1)f (A) almost continuously, whereas the curve for B(1)f (A) itself goes down sharply.
About the authors
S. V. Tolokonnikov
National Research Center Kurchatov Institute; Moscow Institute of Physics and Technology (State University)
Email: saper@mbslab.kiae.ru
Russian Federation, pl. Akademika Kurchatova 1, Moscow, 123182; Institutskii per. 9, Dolgoprudnyi, Moscow oblast, 141700
I. N. Borzov
National Research Center Kurchatov Institute; Joint Institute for Nuclear Research
Email: saper@mbslab.kiae.ru
Russian Federation, pl. Akademika Kurchatova 1, Moscow, 123182; ul. Joliot-Curie 6, Dubna, Moscow oblast, 141980
Yu. S. Lutostansky
National Research Center Kurchatov Institute
Email: saper@mbslab.kiae.ru
Russian Federation, pl. Akademika Kurchatova 1, Moscow, 123182
I. V. Panov
National Research Center Kurchatov Institute; Institute for Theoretical and Experimental Physics
Email: saper@mbslab.kiae.ru
Russian Federation, pl. Akademika Kurchatova 1, Moscow, 123182; Bol’shaya Cheremushkinskaya ul. 25, Moscow, 117218
E. E. Saperstein
National Research Center Kurchatov Institute; National Research Nuclear University MEPhI
Author for correspondence.
Email: saper@mbslab.kiae.ru
Russian Federation, pl. Akademika Kurchatova 1, Moscow, 123182; Kashirskoe sh. 31, Moscow, 115409
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