{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:IT4KRV7COV5LB3JMBTJSLFBBBD","short_pith_number":"pith:IT4KRV7C","schema_version":"1.0","canonical_sha256":"44f8a8d7e2757ab0ed2c0cd325942108cc066b6a440809139a88780489e6cdf9","source":{"kind":"arxiv","id":"2206.06044","version":1},"attestation_state":"computed","paper":{"title":"New measurement of the $E_{\\mathrm{c.m.}}=323$ keV resonance in the $^{19}$F$($p,\\gamma$)$^{20}$Ne reaction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"nucl-ex","authors_text":"A. Lennarz, B. Davids, C. Ruiz, D. Hutcheon, J. Karpesky, M. Lovely, M. Williams, P. Adsley, U. Greife","submitted_at":"2022-06-13T11:08:13Z","abstract_excerpt":"At temperatures below 0.1 GK the $^{19}$F$(p,\\gamma)^{20}$Ne reaction is the only breakout path out of the CNO cycle. Experimental studies of this reaction are challenging from a technical perspective due to copious $\\gamma$-ray background from the far stronger $^{19}$F$(p,\\alpha)^{16}$O reaction channel. Here we present the first inverse kinematics study of the $^{19}$F$(p,\\gamma)^{20}$Ne reaction, in which we measure the strength of the 323-keV resonance. We find a strength value of $\\omega\\gamma = 3.3^{+1.1}_{-0.9}$ meV, which is a factor of two larger than the most recent previous study. T"},"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":"2206.06044","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2022-06-13T11:08:13Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"97e7db46dc23a9ac390b91ca6125ed48457447c9811cb13a0b155fd2ed84674c","abstract_canon_sha256":"fe09bf3909c2eb8f7cd8ee1b296d29c257b558d16d3acee5d310295e46d7986a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:31:14.444265Z","signature_b64":"/GrYmPfsTfEY9SjjsRdZ6yYmz/e0NjEtW2HtV2KxMSYCPR7cIPLXBtQbnyW/9HtF8qLv6vO8ljVLpDh6iZGWAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"44f8a8d7e2757ab0ed2c0cd325942108cc066b6a440809139a88780489e6cdf9","last_reissued_at":"2026-07-05T04:31:14.443856Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:31:14.443856Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New measurement of the $E_{\\mathrm{c.m.}}=323$ keV resonance in the $^{19}$F$($p,\\gamma$)$^{20}$Ne reaction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"nucl-ex","authors_text":"A. Lennarz, B. Davids, C. Ruiz, D. Hutcheon, J. Karpesky, M. Lovely, M. Williams, P. Adsley, U. Greife","submitted_at":"2022-06-13T11:08:13Z","abstract_excerpt":"At temperatures below 0.1 GK the $^{19}$F$(p,\\gamma)^{20}$Ne reaction is the only breakout path out of the CNO cycle. Experimental studies of this reaction are challenging from a technical perspective due to copious $\\gamma$-ray background from the far stronger $^{19}$F$(p,\\alpha)^{16}$O reaction channel. Here we present the first inverse kinematics study of the $^{19}$F$(p,\\gamma)^{20}$Ne reaction, in which we measure the strength of the 323-keV resonance. We find a strength value of $\\omega\\gamma = 3.3^{+1.1}_{-0.9}$ meV, which is a factor of two larger than the most recent previous study. T"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.06044","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2206.06044/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2206.06044","created_at":"2026-07-05T04:31:14.443914+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.06044v1","created_at":"2026-07-05T04:31:14.443914+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.06044","created_at":"2026-07-05T04:31:14.443914+00:00"},{"alias_kind":"pith_short_12","alias_value":"IT4KRV7COV5L","created_at":"2026-07-05T04:31:14.443914+00:00"},{"alias_kind":"pith_short_16","alias_value":"IT4KRV7COV5LB3JM","created_at":"2026-07-05T04:31:14.443914+00:00"},{"alias_kind":"pith_short_8","alias_value":"IT4KRV7C","created_at":"2026-07-05T04:31:14.443914+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/IT4KRV7COV5LB3JMBTJSLFBBBD","json":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD.json","graph_json":"https://pith.science/api/pith-number/IT4KRV7COV5LB3JMBTJSLFBBBD/graph.json","events_json":"https://pith.science/api/pith-number/IT4KRV7COV5LB3JMBTJSLFBBBD/events.json","paper":"https://pith.science/paper/IT4KRV7C"},"agent_actions":{"view_html":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD","download_json":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD.json","view_paper":"https://pith.science/paper/IT4KRV7C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.06044&json=true","fetch_graph":"https://pith.science/api/pith-number/IT4KRV7COV5LB3JMBTJSLFBBBD/graph.json","fetch_events":"https://pith.science/api/pith-number/IT4KRV7COV5LB3JMBTJSLFBBBD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD/action/storage_attestation","attest_author":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD/action/author_attestation","sign_citation":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD/action/citation_signature","submit_replication":"https://pith.science/pith/IT4KRV7COV5LB3JMBTJSLFBBBD/action/replication_record"}},"created_at":"2026-07-05T04:31:14.443914+00:00","updated_at":"2026-07-05T04:31:14.443914+00:00"}