Fission and binary fragmentation reactions in Se-80+Pb-208 and Se-80+Th-232 systems

Fission and binary fragmentation of the excited nuclear systems of Z=116 and 124 were investigated using the reactions induced by Se-80 beams on Pb-208 and Th-232 targets at bombarding energies ranging from 470 to 630 MeV. The mass and kinetic energy of the binary reaction products were reconstructed by measuring their velocities by the time-of-flight method and the angles of emission using multiwire proportional chambers. Total neutron multiplicities were measured in coincidence with the fragments, using an array of neutron detectors. The fragment mass-energy correlation was studied for the two systems. The average total kinetic energy (TKE) of fragments for the Se-80+Pb-208 system agrees with earlier measurements and with Viola's systematics in the mass symmetric region for compound nucleus fission, whereas for the Se-80+Th-232 system, the TKE values are significantly lower. This is also consistent with higher values of total neutron multiplicities observed for the case of Se-80+Th-232 at comparable available energies. From an extrapolation of the measured total neutron multiplicities for the mass symmetric region to zero compound nucleus excitation energy, the average number of prompt neutrons expected to be emitted in the spontaneous fission of the superheavy Z=116 has been estimated to be nu(sf)(tot)=10 +/- 2, which is consistent with the value derived for the same compound nucleus populated in the Fe-56+Th-232 reaction in an earlier work. In the case of the Se-80+Th-232 system, similar analysis was carried out by taking the average TKE from Viola's systematics for estimating the available energy for particle emission corresponding to compound nucleus fission. In this way, by extrapolating the observed neutron multiplicities to zero compound nucleus excitation energy, a value of nu(sf)(tot)=15 +/- 2 was obtained for the spontaneous fission of the superheavy Z=124 nucleus. The increase in the average number of neutrons emitted in fission as a function of the atomic number of the nucleus in the superheavy mass region was confirmed by comparing the results of the present work with published data.