{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:BI7B2CEDTIMC6LWNBWRYDONXER","short_pith_number":"pith:BI7B2CED","schema_version":"1.0","canonical_sha256":"0a3e1d08839a182f2ecd0da381b9b72449d81527d98b5214d4e43af92df1a2fa","source":{"kind":"arxiv","id":"1404.2062","version":1},"attestation_state":"computed","paper":{"title":"Strength of the $E_{\\text{p}}$=1.842 MeV resonance in the $^{40}$Ca(p,$\\gamma$)$^{41}$Sc reaction revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"Andreas Wagner, Antonio Caciolli, Arnd R. Junghans, Daniel Bemmerer, Kai Zuber, Konrad Schmidt, Marie-Luise Menzel, Michael Anders, Mirco Dietz, Ronald Schwengner, Shavkat Akhmadaliev, Zolt\\'an Elekes","submitted_at":"2014-04-08T09:46:31Z","abstract_excerpt":"The strength of the $E_{\\rm p} = 1.842$ MeV resonance in the $^{40}$Ca(p,$\\gamma$)$^{41}$Sc reaction is determined with two different methods: First, by an absolute strength measurement using calcium hydroxide targets, and second, relative to the well-determined strength of the resonance triplet at $E_\\alpha$ = 4.5 MeV in the $^{40}$Ca($\\alpha$,$\\gamma$)$^{44}$Ti reaction. The present new value of $\\omega\\gamma=(0.192\\pm0.017)$ eV is 37% (equivalent to $3.5\\sigma$) higher than the evaluated literature value. In addition, the ratio of the strengths of the 1.842 MeV $^{40}$Ca(p,$\\gamma$)$^{41}$S"},"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":"1404.2062","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2014-04-08T09:46:31Z","cross_cats_sorted":[],"title_canon_sha256":"9904dad24bc62e146f91ca7aee56a9e987c6f451506fcf902f0e8fca1c9ecbf7","abstract_canon_sha256":"103c5d08af5cf3f740990f3e3237b2110d721435e495c7298ede40a7845af6c1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:53:55.669358Z","signature_b64":"3F0QDp3tjGD9p25HsaJd2gJ+m/47PTIUKnsCBGv+EEXAU8HclNQPDcA2Prmohl0qdPjAqwZPD09NtPDFFhIlAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a3e1d08839a182f2ecd0da381b9b72449d81527d98b5214d4e43af92df1a2fa","last_reissued_at":"2026-05-18T02:53:55.668490Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:53:55.668490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strength of the $E_{\\text{p}}$=1.842 MeV resonance in the $^{40}$Ca(p,$\\gamma$)$^{41}$Sc reaction revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"Andreas Wagner, Antonio Caciolli, Arnd R. Junghans, Daniel Bemmerer, Kai Zuber, Konrad Schmidt, Marie-Luise Menzel, Michael Anders, Mirco Dietz, Ronald Schwengner, Shavkat Akhmadaliev, Zolt\\'an Elekes","submitted_at":"2014-04-08T09:46:31Z","abstract_excerpt":"The strength of the $E_{\\rm p} = 1.842$ MeV resonance in the $^{40}$Ca(p,$\\gamma$)$^{41}$Sc reaction is determined with two different methods: First, by an absolute strength measurement using calcium hydroxide targets, and second, relative to the well-determined strength of the resonance triplet at $E_\\alpha$ = 4.5 MeV in the $^{40}$Ca($\\alpha$,$\\gamma$)$^{44}$Ti reaction. The present new value of $\\omega\\gamma=(0.192\\pm0.017)$ eV is 37% (equivalent to $3.5\\sigma$) higher than the evaluated literature value. In addition, the ratio of the strengths of the 1.842 MeV $^{40}$Ca(p,$\\gamma$)$^{41}$S"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.2062","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":"1404.2062","created_at":"2026-05-18T02:53:55.668647+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.2062v1","created_at":"2026-05-18T02:53:55.668647+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.2062","created_at":"2026-05-18T02:53:55.668647+00:00"},{"alias_kind":"pith_short_12","alias_value":"BI7B2CEDTIMC","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_16","alias_value":"BI7B2CEDTIMC6LWN","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_8","alias_value":"BI7B2CED","created_at":"2026-05-18T12:28:22.404517+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/BI7B2CEDTIMC6LWNBWRYDONXER","json":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER.json","graph_json":"https://pith.science/api/pith-number/BI7B2CEDTIMC6LWNBWRYDONXER/graph.json","events_json":"https://pith.science/api/pith-number/BI7B2CEDTIMC6LWNBWRYDONXER/events.json","paper":"https://pith.science/paper/BI7B2CED"},"agent_actions":{"view_html":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER","download_json":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER.json","view_paper":"https://pith.science/paper/BI7B2CED","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.2062&json=true","fetch_graph":"https://pith.science/api/pith-number/BI7B2CEDTIMC6LWNBWRYDONXER/graph.json","fetch_events":"https://pith.science/api/pith-number/BI7B2CEDTIMC6LWNBWRYDONXER/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER/action/storage_attestation","attest_author":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER/action/author_attestation","sign_citation":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER/action/citation_signature","submit_replication":"https://pith.science/pith/BI7B2CEDTIMC6LWNBWRYDONXER/action/replication_record"}},"created_at":"2026-05-18T02:53:55.668647+00:00","updated_at":"2026-05-18T02:53:55.668647+00:00"}