Evaporation residue cross-section in the decay of 254No* formed in 206Pb + 48Ca and its isotopic dependence using other Pb targets within the dynamical cluster-decay model

The dynamical cluster-decay model (DCM), with deformation and orientation effects included, is used to calculate the fusion evaporation residue cross-sections σxnσxn for x=1,2,3 and 4x=1,2,3 and 4 neutrons emission in a fusion reaction 206Pb + 48Ca → 254No* at various 48Ca-beam energies Elab=212.7–242.5 MeVElab=212.7–242.5 MeV (equivalently, E⁎=19.8–43.9 MeVE⁎=19.8–43.9 MeV). Considering the higher multipole deformations up to hexadecapole deformation β4iβ4i and the sticking moment-of-inertia ISIS, the DCM with pocket formula for nuclear proximity potential is shown to give a good description of the measured individual light-particle (here neutrons) decay channels for configurations of “hot, compact” orientations θciθci, within one parameter fitting of the neck-length ΔR  . A check on some of the variables involved in DCM shows that (i) spherical configurations give nearly the same result as above for deformed and oriented ones; (ii) the non-sticking moment-of-inertia INSINS gives unphysical results; and (iii) configurations of “cold, elongated” orientations do not fit the data at all. Furthermore, for the four different isotopes of 204,206,207,208Pb-based reactions, the dependence of, say, the 2n-emission yield σ2nσ2n on the isotopic composition of the compound nucleus is also studied within the DCM for “hot” fusion process. Of all the four Pb-isotopes and three excitation energies E⁎E⁎ considered, at each E⁎E⁎, the ΔR is largest for compound system 256No*, followed by 255No*, 254No* and smallest for 252No*, which means to suggest that the neutrons emission occur earliest for 256No*, then for 255No*, 254No* and finally by 252No*, in complete agreement with experimental data according to which compound system 256No* has the highest cross-section and 252No* the lowest with 255No* and 254No* lying in between. This result is related to the double magicity of both the target (208Pb) and projectile (48Ca) nuclei, as well as to the experimentally known result of projectile with a larger number of neutrons (here the target nucleus Pb) showing an increase in the production cross-section of superheavy nuclei, and is shown to be mainly due to the penetrability factor P in the compound nucleus decay cross-section.