{"paper":{"title":"Realistic effective interactions for halo nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"(2) Institut f\\\"ur Theoretische Physik, Germany), H. M\\\"uther (2), K. Amir-Azimi-Nili (2) ( (1) Department of Physics, Stony Brook, SUNY-Stony Brook, T.T.S. Kuo (1), T\\\"ubingen, Universit\\\"at T\\\"ubingen, USA","submitted_at":"1996-03-29T19:33:41Z","abstract_excerpt":"We study halo nuclei using a two-frequency shell-model approach employing wave functions of two different oscillator constants $\\hbar\\omega_{in}$ and $\\hbar\\omega_{out}$, the former for the inner orbits and the latter for the halo (outer) orbits. An initial application has been made for the halo nuclei $^6$He and $^6$Li, with $0s_{1/2}$ taken as the inner and ( $0p_{3/2}$, $0p_{1/2}$) as the halo orbits. Starting from the Paris NN interaction, we have derived a G-matrix folded-diagram effective interaction for this two-frequency model space, using an essentially exact treatment for the Pauli e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9603045","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}