Self-consistent theory frameworks have been introduced for description of excitations in nuclei at finite temperature, based on energy density functionals formulated using i) relativistic mean field Lagrangian with density dependent meson-nucleon vertex functions, and ii) Skyrme-type functionals. Finite temperature random phase approximation (FTRPA) has been employed in description of multipole excitations and charge-exchange modes. It is shown that in the temperature range T = 1-2 MeV additional transition strength appears at low energies due to thermal unblocking of single-particle orbitals close to the Fermi level. Within the finite temperature Hartree-Fock+RPA based on Skyrme functionals, the electron capture cross sections have been st...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
International audienceThe effect of temperature on the evolution of the isovector dipole and isoscal...
Self-consistent theory frameworks have been introduced for description of excitations in nuclei at f...
International audienceSelf-consistent theory frameworks have been introduced for description of exci...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
The multipole response of nuclei at temperatures T = 0-2 MeV is studied using a self-consistent fini...
The nuclear esponse function of 4°Ca is studied at finite temperature using self-consistent RPA. We ...
The fully self-consistent finite temperature relativistic random phase approximation (FTRRPA) has be...
The relativistic and non-relativistic finite temperature proton-neutron quasiparticle random phase a...
International audienceThe relativistic and nonrelativistic finite temperature proton-neutron quasipa...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
International audienceThe effect of temperature on the evolution of the isovector dipole and isoscal...
Self-consistent theory frameworks have been introduced for description of excitations in nuclei at f...
International audienceSelf-consistent theory frameworks have been introduced for description of exci...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
A fully self-consistent microscopic framework for the evaluation of nuclear weak-interaction rates a...
The multipole response of nuclei at temperatures T = 0-2 MeV is studied using a self-consistent fini...
The nuclear esponse function of 4°Ca is studied at finite temperature using self-consistent RPA. We ...
The fully self-consistent finite temperature relativistic random phase approximation (FTRRPA) has be...
The relativistic and non-relativistic finite temperature proton-neutron quasiparticle random phase a...
International audienceThe relativistic and nonrelativistic finite temperature proton-neutron quasipa...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
The finite temperature Hartree-Fock (FTHF) equations are developed to describe a thermally equilibr...
International audienceThe effect of temperature on the evolution of the isovector dipole and isoscal...