Perturbative Effective Theory in an Oscillator Basis?
arXiv:nucl-th/0204072 · doi:10.1103/PhysRevLett.89.182503
Abstract
The effective interaction/operator problem in nuclear physics is believed to be highly nonperturbative, requiring extended high-momentum spaces for accurate solution. We trace this to difficulties that arise at both short and long distances when the included space is defined in terms of a basis of harmonic oscillator Slater determinants. We show, in the simplest case of the deuteron, that both difficulties can be circumvented, yielding highly perturbative results in the potential even for modest (~6hw) included spaces.
10 pages, 4 figures
References in corpus (2)
Cited by in corpus (20)
- Model-independent low momentum nucleon interaction from phase shift equivalence
- Two-Nucleon Higher Partial-Wave Scattering from Lattice QCD
- Entanglement Rearrangement in Self-Consistent Nuclear Structure Calculations
- Towards grounding nuclear physics in QCD
- Neutrinoless double beta decay in effective field theory: the light Majorana neutrino exchange mechanism
- Lattice methods for strongly interacting many-body systems
- Nucleon-Nucleon Scattering in a Harmonic Potential
- Effective field theory in the harmonic oscillator basis
- Three-fermion problems in optical lattices
- Virial expansion coefficients in the harmonic approximation
- Universal Two-Body Spectra of Ultracold Harmonically Trapped Atoms in Two and Three Dimensions
- Effective Operators for Double-Beta Decay
- Quantum Statistics and Thermodynamics in the Harmonic Approximation
- Effective interactions and operators in no-core shell model
- The Form of the Effective Interaction in Harmonic-Oscillator-Based Effective Theory
- Effective Interactions for the Three-Body Problem
- Nuclear Physics without High-Momentum Potentials: Constructing the Nuclear Effective Interaction Directly from Scattering Observables
- Renormalisation and fixed points in Hilbert Space
- Mapping the Two-Component Atomic Fermi Gas to the Nuclear Shell-Model
- The Shell Model, the Renormalization Group and the Two-Body Interaction