Large basis ab initio shell model investigation of 9-Be and 11-Be
arXiv:nucl-th/0412049 · doi:10.1103/PhysRevC.71.044312
Abstract
We are presenting the first ab initio structure investigation of the loosely bound 11-Be nucleus, together with a study of the lighter isotope 9-Be. The nuclear structure of these isotopes is particularly interesting due to the appearance of a parity-inverted ground state in 11-Be. Our study is performed in the framework of the ab initio no-core shell model. Results obtained using four different, high-precision two-nucleon interactions, in model spaces up to 9\hbarΩ, are shown. For both nuclei, and all potentials, we reach convergence in the level ordering of positive- and negative-parity spectra separately. Concerning their relative position, the positive-parity states are always too high in excitation energy, but a fast drop with respect to the negative-parity spectrum is observed when the model space is increased. This behavior is most dramatic for 11-Be. In the largest model space we were able to reach, the 1/2+ level has dropped down to become either the first or the second excited state, depending on which interaction we use. We also observe a contrasting behavior in the convergence patterns for different two-nucleon potentials, and argue that a three-nucleon interaction is needed to explain the parity inversion. Furthermore, large-basis calculations of 13-C and 11-B are performed. This allows us to study the systematics of the position of the first unnatural-parity state in the N=7 isotone and the A=11 isobar. The 11-B run in the 9\hbarΩmodel space involves a matrix with dimension exceeding 1.1 x 10^9, and is our largest calculation so far. We present results on binding energies, excitation spectra, level configurations, radii, electromagnetic observables, and 10-Be+n overlap functions.
17 pages, 12 figures To be published in Phys. Rev. C Resubmitted version. Minor changes
References in corpus (1)
Cited by in corpus (30)
- Chiral effective field theory and nuclear forces
- The Skyrme Interaction in finite nuclei and nuclear matter
- Recent developments in no-core shell-model calculations
- Nuclear Charge Radii of Be-7,9,10 and the one-neutron halo nucleus Be-11
- Ab Initio Many-Body Calculations of n-3H, n-4He, p-{3,4}He, and n-10Be Scattering
- Coupled-cluster theory for three-body Hamiltonians
- Lattice Simulations for Light Nuclei: Chiral Effective Field Theory at Leading Order
- n-Boson Energies at Finite Volume and Three-Boson Interactions
- Can Ab Initio Theory Explain the Phenomenon of Parity Inversion in Be?
- Infrared length scale and extrapolations for the no-core shell model
- Living on the edge of stability, the limits of the nuclear landscape
- Charge radii and electromagnetic moments of Li and Be isotopes from the ab initio no-core shell model
- Converging sequences in the ab initio no-core shell model
- Resonance parameters of the first 1/2+ state in 9Be and astrophysical implications
- Continuum and Three-Nucleon Force Effects on 9Be Energy Levels
- Ab initio study of the beryllium isotopes Be to Be
- B(E1) Strengths from Coulomb Excitation of 11Be
- Effects of deformation in the three-body structure of 11Li
- Isomeric 0- halo-states in 12Be and 11Li
- Momentum distributions and spectroscopic factors of doubly-closed shell nuclei in correlated basis function theory
- Ground state of medium-heavy doubly-closed shell nuclei in correlated basis function theory
- Formation and decay of resonance state in Be and B nuclei. Microscopic three-cluster model investigations
- Investigation of spectroscopic factors of deeply-bound nucleons in drip-line nuclei with the Gamow shell model
- Coupled-cluster theory for strong entanglement in nuclei
- How to renormalize coupled cluster theory
- The Theory of Nuclear Forces: Is the Never-Ending Story Coming to an End?
- From non-Hermitian effective operators to large-scale no-core shell model calculations for light nuclei
- Recent advances in the theory of nuclear forces
- Ab initio study of the halo structure in Be
- Baryon-Baryon Interactions from the Lattice