We calculate the energy per particle of symmetric nuclearmatter and pure neutronmatter using the many-body Brueckner-Hartree-Fock approach and employing the Chiral Next-To-next-To-next-To leading order (N3LO) nucleon-nucleon (NN) potential, supplemented with various parametrizations of the Chiral Next-To-next-To leading order (N2LO) three-nucleon force. Such combination is able to reproduce several observables of the physics of light nuclei for suitable choices of the parameters entering in the three-nucleon interaction. We find that some of these parametrizations, provide also reasonable values for the observables of nuclear matter at the saturation point
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
We employ modern two- and three-nucleon interactions derived in chiral perturbation theory (ChPT) at...
We employ modern two- and three-nucleon interactions derived in chiral perturbation theory (ChPT) at...
We calculate the energy per particle of symmetric nuclearmatter and pure neutronmatter using the man...
We calculate the energy per particle of symmetric nuclear matter and pure neutron matter using the m...
We calculate the energy per particle of symmetric nuclearmatter and pure neutronmatter using the man...
The energy per particle of symmetric nuclear matter and pure neutron matter is calculated using the ...
The energy per particle of symmetric nuclear matter and pure neutron matter is calculated using the ...
The energy per particle of symmetric nuclear matter and pure neutron matter is calculated using the ...
AbstractThe energy per particle of symmetric nuclear matter and pure neutron matter is calculated us...
Using two-nucleon and three-nucleon interactions derived in the framework of chiral perturbation the...
Using two-nucleon and three-nucleon interactions derived in the framework of chiral perturbation the...
AbstractThe energy per particle of symmetric nuclear matter and pure neutron matter is calculated us...
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
We employ modern two- and three-nucleon interactions derived in chiral perturbation theory (ChPT) at...
We employ modern two- and three-nucleon interactions derived in chiral perturbation theory (ChPT) at...
We calculate the energy per particle of symmetric nuclearmatter and pure neutronmatter using the man...
We calculate the energy per particle of symmetric nuclear matter and pure neutron matter using the m...
We calculate the energy per particle of symmetric nuclearmatter and pure neutronmatter using the man...
The energy per particle of symmetric nuclear matter and pure neutron matter is calculated using the ...
The energy per particle of symmetric nuclear matter and pure neutron matter is calculated using the ...
The energy per particle of symmetric nuclear matter and pure neutron matter is calculated using the ...
AbstractThe energy per particle of symmetric nuclear matter and pure neutron matter is calculated us...
Using two-nucleon and three-nucleon interactions derived in the framework of chiral perturbation the...
Using two-nucleon and three-nucleon interactions derived in the framework of chiral perturbation the...
AbstractThe energy per particle of symmetric nuclear matter and pure neutron matter is calculated us...
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
I calculate the energy per particle of symmetric nuclear matter and pure neutron matter in the frame...
We employ modern two- and three-nucleon interactions derived in chiral perturbation theory (ChPT) at...
We employ modern two- and three-nucleon interactions derived in chiral perturbation theory (ChPT) at...