{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:3IFDDYY6VFCC5S6OKZM7BXGCMA","short_pith_number":"pith:3IFDDYY6","schema_version":"1.0","canonical_sha256":"da0a31e31ea9442ecbce5659f0dcc2601e5d2034314503ca4c0745b41ad5b8b8","source":{"kind":"arxiv","id":"1611.01295","version":2},"attestation_state":"computed","paper":{"title":"Radiative capture reaction for $^{17}$Ne formation within a full three-body model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"E. Garrido, J. Casal, J. M. Arias, M. Rodr\\'iguez-Gallardo, R. de Diego","submitted_at":"2016-11-04T09:38:19Z","abstract_excerpt":"Background: The breakout from the hot Carbon-Nitrogen-Oxigen (CNO) cycles can trigger the rp-process in type I x-ray bursts. In this environment, a competition between $^{15}\\text{O}(\\alpha,\\gamma){^{19}\\text{Ne}}$ and the two-proton capture reaction $^{15}\\text{O}(2p,\\gamma){^{17}\\text{Ne}}$ is expected.\n  Purpose: Determine the three-body radiative capture reaction rate for ${^{17}\\text{Ne}}$ formation including sequential and direct, resonant and non-resonant contributions on an equal footing.\n  Method: Two different discretization methods have been applied to generate $^{17}$Ne states in a"},"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":"1611.01295","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-04T09:38:19Z","cross_cats_sorted":[],"title_canon_sha256":"e712d36507c362fa5452f98d180f31536a0c378cf3e44c723ea4804f508bde27","abstract_canon_sha256":"af6a0f13c903d39dc4e24550d4b6e1a9cd56f08551b9a14d5e2d4a066e01c5ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:56:11.826108Z","signature_b64":"jDVREg+61Iy5Z0LJveMlKNPtJDBWCg4vWjSelyE7R0qX9xMcX1GYSULkmc0r+GO7K3cl08zlCCM5tqAm3V3hDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"da0a31e31ea9442ecbce5659f0dcc2601e5d2034314503ca4c0745b41ad5b8b8","last_reissued_at":"2026-05-18T00:56:11.825644Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:56:11.825644Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative capture reaction for $^{17}$Ne formation within a full three-body model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"E. Garrido, J. Casal, J. M. Arias, M. Rodr\\'iguez-Gallardo, R. de Diego","submitted_at":"2016-11-04T09:38:19Z","abstract_excerpt":"Background: The breakout from the hot Carbon-Nitrogen-Oxigen (CNO) cycles can trigger the rp-process in type I x-ray bursts. In this environment, a competition between $^{15}\\text{O}(\\alpha,\\gamma){^{19}\\text{Ne}}$ and the two-proton capture reaction $^{15}\\text{O}(2p,\\gamma){^{17}\\text{Ne}}$ is expected.\n  Purpose: Determine the three-body radiative capture reaction rate for ${^{17}\\text{Ne}}$ formation including sequential and direct, resonant and non-resonant contributions on an equal footing.\n  Method: Two different discretization methods have been applied to generate $^{17}$Ne states in a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.01295","kind":"arxiv","version":2},"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":"1611.01295","created_at":"2026-05-18T00:56:11.825710+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.01295v2","created_at":"2026-05-18T00:56:11.825710+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.01295","created_at":"2026-05-18T00:56:11.825710+00:00"},{"alias_kind":"pith_short_12","alias_value":"3IFDDYY6VFCC","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_16","alias_value":"3IFDDYY6VFCC5S6O","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_8","alias_value":"3IFDDYY6","created_at":"2026-05-18T12:29:55.572404+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/3IFDDYY6VFCC5S6OKZM7BXGCMA","json":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA.json","graph_json":"https://pith.science/api/pith-number/3IFDDYY6VFCC5S6OKZM7BXGCMA/graph.json","events_json":"https://pith.science/api/pith-number/3IFDDYY6VFCC5S6OKZM7BXGCMA/events.json","paper":"https://pith.science/paper/3IFDDYY6"},"agent_actions":{"view_html":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA","download_json":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA.json","view_paper":"https://pith.science/paper/3IFDDYY6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.01295&json=true","fetch_graph":"https://pith.science/api/pith-number/3IFDDYY6VFCC5S6OKZM7BXGCMA/graph.json","fetch_events":"https://pith.science/api/pith-number/3IFDDYY6VFCC5S6OKZM7BXGCMA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA/action/storage_attestation","attest_author":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA/action/author_attestation","sign_citation":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA/action/citation_signature","submit_replication":"https://pith.science/pith/3IFDDYY6VFCC5S6OKZM7BXGCMA/action/replication_record"}},"created_at":"2026-05-18T00:56:11.825710+00:00","updated_at":"2026-05-18T00:56:11.825710+00:00"}