The difference in the bandhead moments of inertia between the superdeformed (SD) band 194Hg(1) and the two-quasiparticle SD bands 194Hg(2,3) was investigated using the particle-number-conserving treatment for the cran...The difference in the bandhead moments of inertia between the superdeformed (SD) band 194Hg(1) and the two-quasiparticle SD bands 194Hg(2,3) was investigated using the particle-number-conserving treatment for the cranked shell model Hamiltonian, and the pairing interaction strength in SD nuclei is estimated to be much weaker than that in normally deformed nuclei.展开更多
The mass (or binding energy)is one of the fundamental properties of nuclei. Since the first nuclear mass formula was presented by yon Weizsker, more than thirty mass formulae have been proposed. The usual way to check...The mass (or binding energy)is one of the fundamental properties of nuclei. Since the first nuclear mass formula was presented by yon Weizsker, more than thirty mass formulae have been proposed. The usual way to check whether a mass formula展开更多
文摘The difference in the bandhead moments of inertia between the superdeformed (SD) band 194Hg(1) and the two-quasiparticle SD bands 194Hg(2,3) was investigated using the particle-number-conserving treatment for the cranked shell model Hamiltonian, and the pairing interaction strength in SD nuclei is estimated to be much weaker than that in normally deformed nuclei.
文摘The mass (or binding energy)is one of the fundamental properties of nuclei. Since the first nuclear mass formula was presented by yon Weizsker, more than thirty mass formulae have been proposed. The usual way to check whether a mass formula