Effective interactions and operators in no-core shell model
I. Stetcu, J. Rotureau

TL;DR
This paper reviews two approaches—unitary transformations and effective field theory—for constructing effective interactions and operators in the no-core shell model, addressing effects of model space truncation and physical terms in nuclear and atomic systems.
Contribution
It compares and discusses the application of unitary transformation and EFT methods for effective interactions in the NCSM, including recent results and extensions to the Gamow shell model.
Findings
Unitary transformation approach effectively accounts for truncation effects in light nuclei.
EFT-based interactions incorporate symmetries and power counting, applicable to nuclear and atomic systems.
Application of EFT to Gamow shell model extends its usefulness to unbound nuclear states.
Abstract
Solutions to the nuclear many-body problem rely on effective interactions, and in general effective operators, to take into account effects not included in calculations. These include effects due to the truncation to finite model spaces where a numerical calculation is tractable, as well as physical terms not included in the description in the first place. In the no-core shell model (NCSM) framework, we discuss two approaches to the effective interactions based on (i) unitary transformations and (ii) effective field theory (EFT) principles. Starting from a given Hamiltonian, the unitary transformation approach is designed to take into account effects induced by the truncation to finite model spaces in which a numerical calculation is performed. This approach was widely applied to the description of nuclear properties of light nuclei; we review the theory and present representative…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
