The effect of temperature on the evolution of the isovector dipole and isoscalar quadrupole excitations in Ni-68 and Sn-120 nuclei is studied within the fully self-consistent finite temperature quasiparticle random phase approximation framework, based on the Skyrme-type SLy5 energy density functional. The new low-energy excitations emerge due to the transitions from thermally occupied states to the discretized continuum at finite temperatures, whereas the isovector giant dipole resonance is not strongly impacted by the increase of temperature. The radiative dipole strength at low energies is also investigated for the Sn-122 nucleus, becoming compatible with the available experimental data when the temperature is included. In addition, both ...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
The temperature dependence of the energy centroids and strength distributions for Gamow-Teller (GT) ...
Thermal fluctuations of quasiparticle number are included making use of the secondary Bogolyubov's t...
International audienceThe effect of temperature on the evolution of the isovector dipole and isoscal...
The relativistic random phase approximation based on effective Lagrangian with density dependent mes...
The multipole response of nuclei at temperatures T = 0-2 MeV is studied using a self-consistent fini...
International audienceIn the present work, the isovector dipole responses, both in the resonance reg...
In the present work, the isovector dipole responses, both in the resonance region and in the low-ene...
The problem of the damping of the Giant Dipole Resonance (GDR) at finite temperature at T>2 MeV is d...
The description of collective motion in nuclei at finite temperature using the framework of the rand...
The studies of the evolution of the hot Giant Dipole Resonance (GDR) properties as a function of exc...
The theoretical description of nuclear resonances at zero and finite temperatures is presented. The ...
The dipole response function of nuclear matter at zero and finite temperatures is investigated by em...
We study the systematics of the giant dipole resonance width $\Gamma$ in hot rotating nuclei as a fu...
The self-consistent random-phase approximation, based on the framework of relativistic energy densit...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
The temperature dependence of the energy centroids and strength distributions for Gamow-Teller (GT) ...
Thermal fluctuations of quasiparticle number are included making use of the secondary Bogolyubov's t...
International audienceThe effect of temperature on the evolution of the isovector dipole and isoscal...
The relativistic random phase approximation based on effective Lagrangian with density dependent mes...
The multipole response of nuclei at temperatures T = 0-2 MeV is studied using a self-consistent fini...
International audienceIn the present work, the isovector dipole responses, both in the resonance reg...
In the present work, the isovector dipole responses, both in the resonance region and in the low-ene...
The problem of the damping of the Giant Dipole Resonance (GDR) at finite temperature at T>2 MeV is d...
The description of collective motion in nuclei at finite temperature using the framework of the rand...
The studies of the evolution of the hot Giant Dipole Resonance (GDR) properties as a function of exc...
The theoretical description of nuclear resonances at zero and finite temperatures is presented. The ...
The dipole response function of nuclear matter at zero and finite temperatures is investigated by em...
We study the systematics of the giant dipole resonance width $\Gamma$ in hot rotating nuclei as a fu...
The self-consistent random-phase approximation, based on the framework of relativistic energy densit...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
The temperature dependence of the energy centroids and strength distributions for Gamow-Teller (GT) ...
Thermal fluctuations of quasiparticle number are included making use of the secondary Bogolyubov's t...