14 pages, 17 figuresThe hole-state random phase approximation (hRPA) and the particle-state random phase approximation (pRPA) for systems like odd $A$ nuclei are discussed. These hRPA and pRPA are formulated based on the Hartree-Fock ground state. An extension of hRPA and pRPA based on a correlated ground state is given using time-dependent density-matrix theory. Applications to the single-particle states around $^{16}$O are presented. It is shown that inclusion of ground-state correlation affects appreciably the results of hRPA and pRPA. The question of the coupling of the center of mass motion of the core to the particle (hole) is also discussed
International audienceCoupled equations for even and odd particle number correlation functions are s...
The ground states and the first 2+ states of 20O and 22O are derived using two schemes, one consisti...
1 tex, 16 figuresInternational audienceWe make use of a subtraction procedure, introduced to overcom...
14 pages, 17 figuresThe hole-state random phase approximation (hRPA) and the particle-state random p...
Abstract. The Quasi-particle Random Phase Approximation (QRPA) is known to be inade-quate for descri...
Starting from the equations of motion expressed as ground-state expectation values, we have derived ...
We present a new extension of the random-phase approximation method: the quasiboson approximation is...
International audienceWe present an extension of the random-phase approximation (RPA) where the RPA ...
<p>The accurate description of ground and electronic excited states is an important and challenging ...
Second random-phase approximation (RPA) calculations with a Skyrme force are performed to describe b...
We developed a method for computing matrix elements of single-particle operators in the correlated r...
A microscopic formalism is developed that includes the coupling to two particle-hole phonons in the ...
The Faddeev Random Phase Approximation (FRPA) is a Green’s function method which couples collective ...
The random phase approximation (RPA) builds in correlations left out by mean-field theory. In full 0...
It is well known that the Tamm-Dancoff approximation (TDA) is less adequate than the random phase ap...
International audienceCoupled equations for even and odd particle number correlation functions are s...
The ground states and the first 2+ states of 20O and 22O are derived using two schemes, one consisti...
1 tex, 16 figuresInternational audienceWe make use of a subtraction procedure, introduced to overcom...
14 pages, 17 figuresThe hole-state random phase approximation (hRPA) and the particle-state random p...
Abstract. The Quasi-particle Random Phase Approximation (QRPA) is known to be inade-quate for descri...
Starting from the equations of motion expressed as ground-state expectation values, we have derived ...
We present a new extension of the random-phase approximation method: the quasiboson approximation is...
International audienceWe present an extension of the random-phase approximation (RPA) where the RPA ...
<p>The accurate description of ground and electronic excited states is an important and challenging ...
Second random-phase approximation (RPA) calculations with a Skyrme force are performed to describe b...
We developed a method for computing matrix elements of single-particle operators in the correlated r...
A microscopic formalism is developed that includes the coupling to two particle-hole phonons in the ...
The Faddeev Random Phase Approximation (FRPA) is a Green’s function method which couples collective ...
The random phase approximation (RPA) builds in correlations left out by mean-field theory. In full 0...
It is well known that the Tamm-Dancoff approximation (TDA) is less adequate than the random phase ap...
International audienceCoupled equations for even and odd particle number correlation functions are s...
The ground states and the first 2+ states of 20O and 22O are derived using two schemes, one consisti...
1 tex, 16 figuresInternational audienceWe make use of a subtraction procedure, introduced to overcom...