Statistical model and cross sections for the evaporation residues formed in the reaction [formula omitted] at the 22Ne projectile bombarding energy of 6.0–10.0 MeV/nucleon

• Published in: Nuclear physics. A 1997-11, Vol.626 (3), p.857-870, Article 857
• Main Authors: Andreyev, A.N, Bogdanov, D.D, Chepigin, V.I, Kabachenko, A.P, Malyshev, O.N, Oganessian, Yu.Ts, Popeko, A.G, Rohác, J, Sagaidak, R.N, Ter-Akopian, G.M, Yeremin, A.V, Šáro, Š, Veselský, M
• Format: Article
• Language: English
• Subjects: deduced fission barriers. Enriched target, kinematic separator; measured evaporation residue σ( E); NUCLEAR REACTIONS 190Os ( 22Ne, xn),( 22Ne, xnp),( 22Ne, xn α), E = 130–220 MeV; silicon detectors, α-activity measurements
• ISSN: 0375-9474
• DOI: 10.1016/S0375-9474(97)00477-6

The production cross sections were measured for the xn, p xn, and αxn de-excitation channels of the 212Rn compound nuclei formed at excitation energies of 80–160 MeV in the reaction 22Ne + 190Os . The maximum cross sections obtained for the xn ( x = 8–12), p xn ( x = 8–11) and αxn ( x = 8–11) reaction channels were fitted satisfactorily with the computer code HIVAP using its standard parameter set except that the single scaling parameter C = 0.65 was implemented to adjust the values of the liquid-drop fission barriers predicted by the Cohen-Plasil-Swiatecki (CPS) model. Additionally, an analysis of a large set of data on the formation cross sections of neutron-deficient Z = 83–92 nuclei showed that the whole body of data obtained for the nuclear region notable for the large variations of both the liquid-drop barrier and the shell effects, can be described well with practically the same parameter C = 0.55–0.68. One may take this observation as an indication that, though the CPS model overestimates the liquid-drop fission barriers, it reproduces well the relative behaviour of these barriers in the whole range of neutron-deficient Z = 83–92 nuclei.