English

Superdeformed and Hyperdeformed States in Z=122 Isotopes

Nuclear Theory 2009-10-16 v1

Abstract

We calculate the binding energy, root-mean-square radius and quadrupole deformation parameter for the recent, possibly discovered superheavey element Z=122, using the axially deformed relativistic mean field (RMF) and non-relativistic Skyrme Hartree-Fock (SHF) formalisms. The calculation is extended to include various isotopes of Z=122 element, strarting from A=282 to A=320. We predict highly deformed structures in the ground state for all the isotopes. A shape transition appears at about A=290 from a highly oblate to a large prolate shape, which may be considered as the superdeformed and hyperdeformed structures of Z=122 nucleus in the mean field approaches. The most stable isotope (largest binding energy per nucleon) is found to be 302^{302}122, instead of the experimentally observed 292^{292}122.

Keywords

Cite

@article{arxiv.0906.0066,
  title  = {Superdeformed and Hyperdeformed States in Z=122 Isotopes},
  author = {S. K. Patra and M. Bhuyan and M. S. Mehta and Raj K. Gupta},
  journal= {arXiv preprint arXiv:0906.0066},
  year   = {2009}
}

Comments

7 pages 8 Figures 2 Table

R2 v1 2026-06-21T13:07:54.443Z