Add to ORKGConfiguration-constrained calculations of potential-energy surfaces have been performed to study the shape of the K??=7- isomer in 130Ce. The calculated excitation energy agrees well with the experimental data. The resulting deformation indicates that this isomer has a prolate shape as large as that of the ground state. However, the potential-energy surface of the isomeric state is remarkably soft on the ?? degree of freedom, which would be an indication of the K mixing.EI0SUPPL. 2100-1023
We examine the physical conditions, and specifically the role of the quadrupole-octupole deformation...
Excited states of the N=Z=33 nucleus 66As have been populated in a fusion-evaporation reaction and s...
Excited states of the N=Z=33 nucleus 66As have been populated in a fusion-evaporation reaction and s...
Configuration-constrained calculations of potential-energy surfaces have been performed to study the...
A partial decay scheme for Xe is presented. The K = 8 state is isomeric with a half-life of 73(5) ns...
To determine which nuclei may exhibit shape isomerism, we use a well-benchmarked macroscopic-microsc...
In the past years, we have made many theoretical investigations on multi-quasiparticle high-K isomer...
In the past years, we have made many theoretical investigations on multi-quasiparticle high-K isomer...
Isomeric states in the nuclei along the rapid proton capture process path are studied by the project...
Shape coexistence in the light krypton isotopes was studied in a series of experiments at GANIL usin...
Shape coexistence in the light krypton isotopes was studied in a series of experiments at GANIL usin...
A partial decay scheme for 128Xe is presented. The Kπ = 8- state is isomeric with a half-life of 73(...
Structures above the two-particle isomeric states in 188Pb have been identified. Their properties im...
A proper treatment of K-mixing is the key to understanding K-isomers. Here, we present a method base...
We calculate potential-energy surfaces as functions of spheroidal (epsilon(2)), hexadecapole (epsilo...
We examine the physical conditions, and specifically the role of the quadrupole-octupole deformation...
Excited states of the N=Z=33 nucleus 66As have been populated in a fusion-evaporation reaction and s...
Excited states of the N=Z=33 nucleus 66As have been populated in a fusion-evaporation reaction and s...
Configuration-constrained calculations of potential-energy surfaces have been performed to study the...
A partial decay scheme for Xe is presented. The K = 8 state is isomeric with a half-life of 73(5) ns...
To determine which nuclei may exhibit shape isomerism, we use a well-benchmarked macroscopic-microsc...
In the past years, we have made many theoretical investigations on multi-quasiparticle high-K isomer...
In the past years, we have made many theoretical investigations on multi-quasiparticle high-K isomer...
Isomeric states in the nuclei along the rapid proton capture process path are studied by the project...
Shape coexistence in the light krypton isotopes was studied in a series of experiments at GANIL usin...
Shape coexistence in the light krypton isotopes was studied in a series of experiments at GANIL usin...
A partial decay scheme for 128Xe is presented. The Kπ = 8- state is isomeric with a half-life of 73(...
Structures above the two-particle isomeric states in 188Pb have been identified. Their properties im...
A proper treatment of K-mixing is the key to understanding K-isomers. Here, we present a method base...
We calculate potential-energy surfaces as functions of spheroidal (epsilon(2)), hexadecapole (epsilo...
We examine the physical conditions, and specifically the role of the quadrupole-octupole deformation...
Excited states of the N=Z=33 nucleus 66As have been populated in a fusion-evaporation reaction and s...
Excited states of the N=Z=33 nucleus 66As have been populated in a fusion-evaporation reaction and s...