Solving the two-center nuclear shell-model problem with arbitrarily-orientated deformed potentials
arXiv:0810.0353 · doi:10.1103/PhysRevLett.101.122501
Abstract
A general new technique to solve the two-center problem with arbitrarily-orientated deformed realistic potentials is demonstrated, which is based on the powerful potential separable expansion method. As an example, molecular single-particle spectra for C + C Mg are calculated using deformed Woods-Saxon potentials. These clearly show that non-axial symmetric configurations play a crucial role in molecular resonances observed in reaction processes for this system at low energy.
References in corpus (7)
- Deformed two center shell model
- Evaluation of Spectra of Baryons Containing Two Heavy Quarks in Bag Model
- Two center shell model with Woods-Saxon potentials: adiabatic and diabatic states in fusion
- Effects of nuclear molecular configurations on the astrophysical S-factor for O + O
- Modelling of compound nucleus formation in fusion of heavy nuclei
- Shell corrections for finite depth potentials with bound states only
- Alpha particle production by molecular single-particle effect in reactions of Be just above the Coulomb barrier
Cited by in corpus (10)
- Multidimensionally-constrained covariant density functional theories --- nuclear shapes and potential energy surfaces
- The effect of 12C + 12C rate uncertainties on the evolution and nucleosynthesis of massive stars
- Characterizing the astrophysical S-factor for C+C with wave-packet dynamics
- New dynamical pair breaking effect
- Pairing gaps and Fermi energies at scission for 296Lv alpha-decay
- Role of continuum in nuclear direct reactions with one-neutron halo nuclei: a one-dimensional model
- Combined few-body and mean-field model for nuclei
- Tracing the dynamical interplay of low-energy reaction processes of exotic nuclei using a two-center molecular continuum
- New and efficient method for solving the eigenvalue problem for the two-center shell model with finite-depth potentials
- Two-center harmonic oscillator basis for Skyrme-DFT calculations (I): formalism and Proof of Principle