{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:WVURT7I6BJYTDRW4FUVHPKGF24","short_pith_number":"pith:WVURT7I6","schema_version":"1.0","canonical_sha256":"b56919fd1e0a7131c6dc2d2a77a8c5d72e687ccc45d60ac59faaaf8f0f76ad6b","source":{"kind":"arxiv","id":"1707.02135","version":1},"attestation_state":"computed","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"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1707.02135","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-07-07T12:02:21Z","cross_cats_sorted":[],"title_canon_sha256":"7fa107da433b915140a15e168f8a75956e49c2fcd0abce188a2aeeef85a979de","abstract_canon_sha256":"8d5332dbb772dbf145ec6ddf906c16a3e5f403acff6a29227b1d9f28a5445273"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:42.825917Z","signature_b64":"P87HfUpQwpZL6FkGjcmDjkGTZu+WjxIzLza0xVY0liwjxFeGslNATwFfIbt5lD8dEsZ232UoL//FIGtCiVE4AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b56919fd1e0a7131c6dc2d2a77a8c5d72e687ccc45d60ac59faaaf8f0f76ad6b","last_reissued_at":"2026-05-18T00:40:42.825165Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:42.825165Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1707.02135","created_at":"2026-05-18T00:40:42.825289+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.02135v1","created_at":"2026-05-18T00:40:42.825289+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.02135","created_at":"2026-05-18T00:40:42.825289+00:00"},{"alias_kind":"pith_short_12","alias_value":"WVURT7I6BJYT","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"WVURT7I6BJYTDRW4","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"WVURT7I6","created_at":"2026-05-18T12:31:53.515858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24","json":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24.json","graph_json":"https://pith.science/api/pith-number/WVURT7I6BJYTDRW4FUVHPKGF24/graph.json","events_json":"https://pith.science/api/pith-number/WVURT7I6BJYTDRW4FUVHPKGF24/events.json","paper":"https://pith.science/paper/WVURT7I6"},"agent_actions":{"view_html":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24","download_json":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24.json","view_paper":"https://pith.science/paper/WVURT7I6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.02135&json=true","fetch_graph":"https://pith.science/api/pith-number/WVURT7I6BJYTDRW4FUVHPKGF24/graph.json","fetch_events":"https://pith.science/api/pith-number/WVURT7I6BJYTDRW4FUVHPKGF24/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24/action/storage_attestation","attest_author":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24/action/author_attestation","sign_citation":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24/action/citation_signature","submit_replication":"https://pith.science/pith/WVURT7I6BJYTDRW4FUVHPKGF24/action/replication_record"}},"created_at":"2026-05-18T00:40:42.825289+00:00","updated_at":"2026-05-18T00:40:42.825289+00:00"}