Gamow Shell-Model Description of Weakly Bound and Unbound Nuclear States
arXiv:nucl-th/0401036 · doi:10.1140/epjad/i2005-06-136-7
Abstract
Recently, the shell model in the complex k-plane (the so-called Gamow Shell Model) has been formulated using a complex Berggren ensemble representing bound single-particle states, single-particle resonances, and non-resonant continuum states. In this framework, we shall discuss binding energies and energy spectra of neutron-rich helium and lithium isotopes. The single-particle basis used is that of the Hartree-Fock potential generated self-consistently by the finite-range residual interaction.
13 pages, 2 figures, presented by N. Michel at the XXVII Symposium On Nuclear Physics, Taxco, Guerrero, Mexico, January 5-8 2004
References in corpus (5)
- Gamow Shell Model Description of Weakly Bound Nuclei and Unbound Nuclear States
- Three-body monopole corrections to the realistic interactions
- Proton-Neutron Coupling in the Gamow Shell Model: the Lithium Chain
- Shell model in the complex energy plane and two-particle resonances
- Microscopic Nuclear Structure Based upon a Chiral NN Potential
Cited by in corpus (7)
- Effective Field Theory and the Gamow Shell Model: The 6He Halo Nucleus
- Neutron Transfer reactions induced by 8Li on 9Be
- A simple and efficient numerical scheme to integrate non-local potentials
- Gamow Shell Model description of Li isotopes and their mirror partners
- Spectroscopic factors of resonance states with the Gamow shell model
- Nuclear structure far from stability
- The Analytic Continuation of the Lippmann-Schwinger Eigenfunctions, and Antiunitary Symmetries