{"paper":{"title":"Spin-tensor decomposition of nuclear transition matrix elements for neutrinoless double-$\\beta $ decay of $^{76}$Ge and $^{82}$Se nuclei within PHFB approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Kumar, B. M. Dixit, P. K. Raina, P. K. Rath, R. Chandra","submitted_at":"2017-07-07T12:02:21Z","abstract_excerpt":"Employing the PHFB model, nuclear transition matrix elements $M^{\\left( K\\right) }$ for the neutrinoless double-$\\beta^{-} $ decay of $\\ ^{76}$Ge and $^{82}$Se isotopes are calculated within mechanisms involving light as well as heavy Majorana neutrinos, and classical Majorons by considering the spin-tensor decomposition of realistic KUO and empirical JUN45 effective two-body interaction. It is noticed that the effects due to the SRC on NTMEs $M^{\\left( 0\\nu \\right) }$ and $M^{\\left( 0N\\right) }$ due to the exchange of light and heavy Majorana neutrinos, respectively, is maximally incorporated"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.02135","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"}