The series of high-K multiquasiparticle bands in Hf-172,Hf-173,Hf-174,Hf-175 are investigated using the particle-number-conserving (PNC) method for treating the cranked shell model with monopole and quadrupole pairing interactions. The experimental results, including the moments of inertia and angular momentum alignments relative to the ground state band Hf-172(g.s.b.) are reproduced quite well by the PNC calculation, in which no free parameter is involved. The difference in the omega variation of the moments of inertia between the high-K multiquasiparticle bands and Hf-172(g.s.b.) is mainly due to the blocking effects of high j intruder orbitals near the Fermi surface. The omega variation of the occupation probability of each cranked orbit...
The microscopic mechanism of the identical bands in odd-odd nucleus Tl-194 and its neighbor odd-A nu...
The microscopic mechanism of the identical bands in odd-odd nucleus 194Tl and its neighbor odd-A nuc...
The variations in moments of inertia (J((2)) and J((1))) with rotational frequency for the series of...
Using the particle-number conserving method for treating the cranked shell model, the microscopic me...
Using the particle-number conserving (PNC) method for treating the cranked shell model, the microsco...
The K = 1/2 rotational band in Yb-171 is investigated using the particle number conserving (PNC) met...
The variations of moments of inertia of superdeformed (SD) bands Hg-194(1) and Hg-192(1) With angula...
The omega variation of moments of inertia of superdeformed bands is investigated by a particle-numbe...
Using the Particle-number Conserving (PNC) method for treating the cranked shell model, the high K m...
Using the particle-number conserving method for treating the cranked shell model, the microscopic me...
The experimental one-, three-, and five-quasiparticle bands in Ta-179 are analyzed by the particle-n...
Within the framework of the particle-number conserving (PNC) formalism, one-quasiparticle and low-ly...
The experimental high-K 2- and 3-quasiparticle bands of well deformed rare-earth nuclei are analyzed...
Using the Particle-number Conserving (PNC) method for treating the cranked shell model, the high K m...
The experimental one-, three-, and five-quasiparticle bands in Lu-177 are analyzed by the particle-n...
The microscopic mechanism of the identical bands in odd-odd nucleus Tl-194 and its neighbor odd-A nu...
The microscopic mechanism of the identical bands in odd-odd nucleus 194Tl and its neighbor odd-A nuc...
The variations in moments of inertia (J((2)) and J((1))) with rotational frequency for the series of...
Using the particle-number conserving method for treating the cranked shell model, the microscopic me...
Using the particle-number conserving (PNC) method for treating the cranked shell model, the microsco...
The K = 1/2 rotational band in Yb-171 is investigated using the particle number conserving (PNC) met...
The variations of moments of inertia of superdeformed (SD) bands Hg-194(1) and Hg-192(1) With angula...
The omega variation of moments of inertia of superdeformed bands is investigated by a particle-numbe...
Using the Particle-number Conserving (PNC) method for treating the cranked shell model, the high K m...
Using the particle-number conserving method for treating the cranked shell model, the microscopic me...
The experimental one-, three-, and five-quasiparticle bands in Ta-179 are analyzed by the particle-n...
Within the framework of the particle-number conserving (PNC) formalism, one-quasiparticle and low-ly...
The experimental high-K 2- and 3-quasiparticle bands of well deformed rare-earth nuclei are analyzed...
Using the Particle-number Conserving (PNC) method for treating the cranked shell model, the high K m...
The experimental one-, three-, and five-quasiparticle bands in Lu-177 are analyzed by the particle-n...
The microscopic mechanism of the identical bands in odd-odd nucleus Tl-194 and its neighbor odd-A nu...
The microscopic mechanism of the identical bands in odd-odd nucleus 194Tl and its neighbor odd-A nuc...
The variations in moments of inertia (J((2)) and J((1))) with rotational frequency for the series of...