4.5 Article

Deuteron-equivalent and phase-equivalent interactions within light nuclei

Journal

PHYSICAL REVIEW C
Volume 85, Issue 3, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevC.85.034004

Keywords

-

Funding

  1. US DOE [DE-FC02-09ER41582, DE-FG02-87ER40371]
  2. Ministry of Education and Science of the Russian Federation [P521]
  3. Direct For Computer & Info Scie & Enginr
  4. Office of Advanced Cyberinfrastructure (OAC) [0904782] Funding Source: National Science Foundation

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Background: Phase-equivalent transformations (PETs) are well known in quantum scattering and inverse-scattering theory. PETs do not affect scattering phase shifts and bound-state energies of a two-body system but are conventionally supposed to modify two-body bound-state observables such as the rms radius and electromagnetic moments. Purpose: In order to preserve all bound-state observables, we propose a new particular case of PETs, a deuteron-equivalent transformation (DET-PET), which leaves unchanged not only scattering phase shifts and bound-state (deuteron) binding energy but also the bound-state wave function. Methods: The construction of DET-PET is discussed; equations defining the simplest DET-PETs are derived. We apply these simplest DET-PETs to the JISP16 NN interaction and use the transformed NN interactions in calculations of H-3 and He-4 binding energies in the no-core full configuration (NCFC) approach based on extrapolations of the no-core shell model (NCSM) basis space results to the infinite basis space. Results: We demonstrate the DET-PET modification of the np scattering wave functions and study the DET-PET manifestation in the binding energies of H-3 and He-4 nuclei and their correlation (Tjon line). Conclusions: It is shown that some DET-PETs generate modifications of the central component while the others modify the tensor component of the NN interaction. DET-PETs are able to modify significantly the np scattering wave functions and hence the off-shell properties of the NN interaction. DET-PETs give rise to significant changes in the binding energies of H-3 (in the range of approximately 1.5 MeV) and He-4 (in the range of more than 9 MeV) and are able to modify the correlation patterns of binding energies of these nuclei.

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