{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:PTJU6CPRQ6SZKGXCJCHARZTIG4","short_pith_number":"pith:PTJU6CPR","schema_version":"1.0","canonical_sha256":"7cd34f09f187a5951ae2488e08e668372a139e70c063be1efa3a6f20ab326c3f","source":{"kind":"arxiv","id":"1507.07442","version":1},"attestation_state":"computed","paper":{"title":"Large scale evaluation of beta-decay rates of r-process nuclei with the inclusion of first-forbidden transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","nucl-ex"],"primary_cat":"nucl-th","authors_text":"G. Mart\\'inez-Pinedo, L. Huther, T. Marketin","submitted_at":"2015-07-27T15:18:04Z","abstract_excerpt":"R-process nucleosynthesis models rely, by necessity, on nuclear structure models for input. Particularly important are beta-decay half-lives of neutron rich nuclei. At present only a single systematic calculation exists that provides values for all relevant nuclei making it difficult to test the sensitivity of nucleosynthesis models to this input. Additionally, even though there are indications that their contribution may be significant, the impact of first-forbidden transitions on decay rates has not been systematically studied within a consistent model. We use a fully self-consistent covaria"},"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":"1507.07442","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-27T15:18:04Z","cross_cats_sorted":["astro-ph.HE","nucl-ex"],"title_canon_sha256":"f292fd56ca0073fc3ef1b7ed7b6e785ae4e61440556995aadb7f8dc7fa032a9c","abstract_canon_sha256":"1dd378be8c179f2cd45e8cc5ff65aca66097133e0b22c0c8c9524b9a4dca09c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:46.250727Z","signature_b64":"hnBsq5cJgDRYw3g4pJqOQHpOCbtBRHY2eTWbJraKHIVg3XLb9/WCDtRb6fVotK67BGWx0bnUzjhrsi05kugdDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7cd34f09f187a5951ae2488e08e668372a139e70c063be1efa3a6f20ab326c3f","last_reissued_at":"2026-05-18T01:09:46.250013Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:46.250013Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large scale evaluation of beta-decay rates of r-process nuclei with the inclusion of first-forbidden transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","nucl-ex"],"primary_cat":"nucl-th","authors_text":"G. Mart\\'inez-Pinedo, L. Huther, T. Marketin","submitted_at":"2015-07-27T15:18:04Z","abstract_excerpt":"R-process nucleosynthesis models rely, by necessity, on nuclear structure models for input. Particularly important are beta-decay half-lives of neutron rich nuclei. At present only a single systematic calculation exists that provides values for all relevant nuclei making it difficult to test the sensitivity of nucleosynthesis models to this input. Additionally, even though there are indications that their contribution may be significant, the impact of first-forbidden transitions on decay rates has not been systematically studied within a consistent model. We use a fully self-consistent covaria"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.07442","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":"1507.07442","created_at":"2026-05-18T01:09:46.250110+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.07442v1","created_at":"2026-05-18T01:09:46.250110+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.07442","created_at":"2026-05-18T01:09:46.250110+00:00"},{"alias_kind":"pith_short_12","alias_value":"PTJU6CPRQ6SZ","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_16","alias_value":"PTJU6CPRQ6SZKGXC","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_8","alias_value":"PTJU6CPR","created_at":"2026-05-18T12:29:37.295048+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.17213","citing_title":"Identifying observable MeV lines from the decays of weak and main $r$-process isotopes in mergers","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2605.11074","citing_title":"Observational Signatures and Constraints on the Intermediate Neutron-Capture Process. The Case of the CEMP star TYC 6044-714-1 (RAVE J094921.8-161722)","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2507.09040","citing_title":"R-process heating implementation in hydrodynamic simulations with neural networks","ref_index":89,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4","json":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4.json","graph_json":"https://pith.science/api/pith-number/PTJU6CPRQ6SZKGXCJCHARZTIG4/graph.json","events_json":"https://pith.science/api/pith-number/PTJU6CPRQ6SZKGXCJCHARZTIG4/events.json","paper":"https://pith.science/paper/PTJU6CPR"},"agent_actions":{"view_html":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4","download_json":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4.json","view_paper":"https://pith.science/paper/PTJU6CPR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.07442&json=true","fetch_graph":"https://pith.science/api/pith-number/PTJU6CPRQ6SZKGXCJCHARZTIG4/graph.json","fetch_events":"https://pith.science/api/pith-number/PTJU6CPRQ6SZKGXCJCHARZTIG4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4/action/storage_attestation","attest_author":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4/action/author_attestation","sign_citation":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4/action/citation_signature","submit_replication":"https://pith.science/pith/PTJU6CPRQ6SZKGXCJCHARZTIG4/action/replication_record"}},"created_at":"2026-05-18T01:09:46.250110+00:00","updated_at":"2026-05-18T01:09:46.250110+00:00"}