ar X iv : n uc l - th / 9 51 10 37 v 1 2 9 N ov 1 99 5 Z = 110 – 111 Elements and the Stability of Heavy and Superheavy Elements

ar X iv : n uc l - th / 9 60 80 20 v 1 1 2 A ug 1 99 6 Shell Structure of the Superheavy Elements

Ground state properties of the superheavy elements (SHE) with 108≤Z≤128 and 150≤N ≤192 are investigated using both the Skyrme-Hartree-Fock method with a density-independent contact pairing interaction and the macroscopic-microscopic approach with an average Woods-Saxon potential and a monopole pairing interaction. Detailed analysis of binding energies, separation energies, shell effects, single...

ar X iv : n uc l - th / 9 70 40 15 v 1 9 A pr 1 99 7 Microscopic Enhancement of Heavy - Element Production

Realistic fusion barriers are calculated in a macroscopic-microscopic model for several soft-fusion heavy-ion reactions leading to heavy and superheavy elements. The results obtained in such a realistic picture are very different from those obtained in a purely macroscopic model. For reactions on 208 Pb targets, shell effects in the entrance channel result in fusion-barrier energies at the touc...

ar X iv : n uc l - th / 9 60 80 57 v 2 1 8 N ov 1 99 6 Strong decays of nonstrange q 3 baryons

ar X iv : n uc l - th / 9 50 80 39 v 1 2 3 A ug 1 99 5 Collisions of Deformed Nuclei and Superheavy - Element Production

A detailed understanding of complete fusion cross sections in heavy-ion collisions requires a consideration of the effects of the deformation of the projectile and target. Our aim here is to show that deformation and orientation of the colliding nuclei have a very significant effect on the fusion-barrier height and on the compactness of the touching configuration. To facilitate discussions of f...

ar X iv : n uc l - th / 9 71 10 31 v 1 1 8 N ov 1 99 7 HUPD - 9722 Effect of ρN channel in the γN → ππN reactions