Chiral pion-nucleon dynamics in finite nuclei: spin-isospin excitations
arXiv:nucl-th/0612026 · doi:10.1016/j.nuclphysa.2007.04.007
Abstract
The nuclear density functional framework, based on chiral dynamics and the symmetry breaking pattern of low-energy QCD, is extended to the description of collective nuclear excitations. Starting from the relativistic point-coupling Lagrangian previously introduced [Nucl. Phys. A770 (2006) 1], the proton-neutron (quasiparticle) random phase approximation is formulated and applied to investigate the role of chiral pion-nucleon dynamics in excitation modes involving spin and isospin degrees of freedom, e.g. isobaric analog states and Gamow-Teller resonances.
arXiv comment17 pages, 6 figures, elsart class. Minor revisions, Nuclear Physics A in print
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Cited by in corpus (13)
- Toward ab initio density functional theory for nuclei
- Spin-orbit and tensor mean-field effects on spin-orbit splitting including self-consistent core polarizations
- Self-consistent relativistic quasiparticle random-phase approximation and its applications to charge-exchange excitations and -decay half-lives
- Spin-isospin nuclear response using the existing microscopic Skyrme functionals
- Feasibility of the finite amplitude method in covariant density functional theory
- Nuclear /EC decays in covariant density functional theory and the impact of isoscalar proton-neutron pairing
- Nuclear -decay half-lives in the relativistic point-coupling model
- Hypernuclear single particle spectra based on in-medium chiral SU(3) dynamics
- Nuclear charge-exchange excitations based on relativistic density-dependent point-coupling model
- The quest for novel modes of excitation in exotic nuclei
- In-medium chiral SU(3) dynamics and hypernuclear structure
- Nuclear Energy Density Functionals Constrained by Low-Energy QCD
- Point-Coupling Models from Mesonic Hypermassive Limit and Mean-Field Approaches