{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:GUVHAB2IL2N6RJLIDULIZCNFRE","short_pith_number":"pith:GUVHAB2I","schema_version":"1.0","canonical_sha256":"352a7007485e9be8a5681d168c89a58927b2815585ce47131ce3d7acedc1fc8e","source":{"kind":"arxiv","id":"1112.5786","version":1},"attestation_state":"computed","paper":{"title":"Q-Value and Half-Lives for the Double-Beta-Decay Nuclide 110Pd","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Herlert, Ch. B\\\"ohm, Ch. Borgmann, D. Beck, D. Fink, D. Lunney, F. Herfurth, F. Simkovic, J. Barea, J. Kotila, J. Stanja, K. Blaum, K. Zuber, L. Schweikhard, M. Breitenfeldt, M. Kowalska, M. Rosenbusch, S. Kreim, S. Naimi, S. Schwarz","submitted_at":"2011-12-25T17:19:22Z","abstract_excerpt":"The 110Pd double-beta decay Q-value was measured with the Penning-trap mass spectrometer ISOLTRAP to be Q = 2017.85(64) keV. This value shifted by 14 keV compared to the literature value and is 17 times more precise, resulting in new phase-space factors for the two-neutrino and neutrinoless decay modes. In addition a new set of the relevant matrix elements has been calculated. The expected half-life of the two-neutrino mode was reevaluated as 1.5(6) E20 yr. With its high natural abundance, the new results reveal 110Pd to be an excellent candidate for double-beta decay studies."},"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":"1112.5786","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-12-25T17:19:22Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"5a96fdf721cdaa362281446602d092ccb8db98df60b6b232d9c45e1bbb0a3888","abstract_canon_sha256":"485d51b47838f7f2a40d61d3a21ba00ce1bdb3d294bc4015a52bc8f05a1321e1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:00.667941Z","signature_b64":"FJlwNPHa7aODYcROladWAXcqyafpDnVN/o3PR0bw8alxtdozj8xs0Wv/NciN1mS79vQkhDtMa2GZwzSnm65rDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"352a7007485e9be8a5681d168c89a58927b2815585ce47131ce3d7acedc1fc8e","last_reissued_at":"2026-05-18T01:59:00.667246Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:00.667246Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Q-Value and Half-Lives for the Double-Beta-Decay Nuclide 110Pd","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Herlert, Ch. B\\\"ohm, Ch. Borgmann, D. Beck, D. Fink, D. Lunney, F. Herfurth, F. Simkovic, J. Barea, J. Kotila, J. Stanja, K. Blaum, K. Zuber, L. Schweikhard, M. Breitenfeldt, M. Kowalska, M. Rosenbusch, S. Kreim, S. Naimi, S. Schwarz","submitted_at":"2011-12-25T17:19:22Z","abstract_excerpt":"The 110Pd double-beta decay Q-value was measured with the Penning-trap mass spectrometer ISOLTRAP to be Q = 2017.85(64) keV. This value shifted by 14 keV compared to the literature value and is 17 times more precise, resulting in new phase-space factors for the two-neutrino and neutrinoless decay modes. In addition a new set of the relevant matrix elements has been calculated. The expected half-life of the two-neutrino mode was reevaluated as 1.5(6) E20 yr. With its high natural abundance, the new results reveal 110Pd to be an excellent candidate for double-beta decay studies."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.5786","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":"1112.5786","created_at":"2026-05-18T01:59:00.667354+00:00"},{"alias_kind":"arxiv_version","alias_value":"1112.5786v1","created_at":"2026-05-18T01:59:00.667354+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.5786","created_at":"2026-05-18T01:59:00.667354+00:00"},{"alias_kind":"pith_short_12","alias_value":"GUVHAB2IL2N6","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_16","alias_value":"GUVHAB2IL2N6RJLI","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_8","alias_value":"GUVHAB2I","created_at":"2026-05-18T12:26:30.835961+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/GUVHAB2IL2N6RJLIDULIZCNFRE","json":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE.json","graph_json":"https://pith.science/api/pith-number/GUVHAB2IL2N6RJLIDULIZCNFRE/graph.json","events_json":"https://pith.science/api/pith-number/GUVHAB2IL2N6RJLIDULIZCNFRE/events.json","paper":"https://pith.science/paper/GUVHAB2I"},"agent_actions":{"view_html":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE","download_json":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE.json","view_paper":"https://pith.science/paper/GUVHAB2I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1112.5786&json=true","fetch_graph":"https://pith.science/api/pith-number/GUVHAB2IL2N6RJLIDULIZCNFRE/graph.json","fetch_events":"https://pith.science/api/pith-number/GUVHAB2IL2N6RJLIDULIZCNFRE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE/action/storage_attestation","attest_author":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE/action/author_attestation","sign_citation":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE/action/citation_signature","submit_replication":"https://pith.science/pith/GUVHAB2IL2N6RJLIDULIZCNFRE/action/replication_record"}},"created_at":"2026-05-18T01:59:00.667354+00:00","updated_at":"2026-05-18T01:59:00.667354+00:00"}