International Journal of Modern Physics E · 2011 · 10 citations · 8 references
Natural SciencesPhysicsNuclear PhysicsParticle PhysicsQuantum MechanicsHartree-fock TheoryNuclear Binding EnergyNuclear ForcesNuclear ModelsNuclear StructureStrong InteractionGround State PropertiesHamiltonian FormulationIsospin Dependence Of Few-body InteractionsIsospin PhysicsMany-body CorrelationsMany-body DynamicsMany-body Nuclear ForcesNuclear Pairing Correlations
In self-consistent mean-field approaches, the description of odd-mass nuclei requires to break the time-reversal invariance of the underlying one-body hamiltonian. This induces a polarization of the even-even core to which the odd nucleon is added. To properly describe the pairing correlations (in T = 1 and T = 0 channels) in such nuclei, we implement the particle-number conserving Higher Tamm–Dancoff approximation with a residual δ interaction in each isospin channel by restricting the many-body basis to two-particle–two–hole excitations of pair type (nn, pp and np) on top of the Hartree–Fock solution. We apply this approach to the calculation of two ground-state properties of well-deformed nuclei |T z | = 1 nuclei around 24 Mg and 48 Cr , namely the isovector odd-even binding-energy difference and the magnetic dipole moment, focusing on the impact of pairing correlations.
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