{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:M7TBGALBC6LQ3RM2DY6FB7SILZ","short_pith_number":"pith:M7TBGALB","schema_version":"1.0","canonical_sha256":"67e613016117970dc59a1e3c50fe485e63bfbdfd6d3add841953fa201d27d2a1","source":{"kind":"arxiv","id":"1507.01828","version":3},"attestation_state":"computed","paper":{"title":"Capture reactions into borromean two-proton systems at rp-waiting points","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"nucl-th","authors_text":"A.S. Jensen, D. Hove, D.V. Fedorov, E. Garrido, H.O.U. Fynbo, N.T. Zinner","submitted_at":"2015-07-07T14:45:19Z","abstract_excerpt":"We investigate even-even two-proton borromean systems at prominent intermediate heavy waiting points for the rapid proton capture process. The most likely single-particle levels are used to calculate three-body energy and structure as a function of proton-core resonance energy. We establish a linear dependence between two- and three-body energies with the same slope, but the absolute value slightly dependent on partial wave structure. Using these relations we predict low-lying excited states in the isotones following the critical waiting points. The capture rate for producing a borromean bound"},"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":"1507.01828","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-07T14:45:19Z","cross_cats_sorted":["astro-ph.HE"],"title_canon_sha256":"30d445ffca7e2fd7f734774b862b93293fdcb23254d4352a77436a3f14081b44","abstract_canon_sha256":"cc2080fc6607fecf3b2cfee3b42046dace0f0e2fd8788e361053d4cb2ede7d47"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:31.913534Z","signature_b64":"gjIL7i3ACny9RnfQkx6/AqRHoVgIGrLTCvSw0pvuILFEdUSVTFi9CxTmzUlyKLiwTCSccc7bvYGa9gyUNiWuDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67e613016117970dc59a1e3c50fe485e63bfbdfd6d3add841953fa201d27d2a1","last_reissued_at":"2026-05-18T01:21:31.912779Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:31.912779Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Capture reactions into borromean two-proton systems at rp-waiting points","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"nucl-th","authors_text":"A.S. Jensen, D. Hove, D.V. Fedorov, E. Garrido, H.O.U. Fynbo, N.T. Zinner","submitted_at":"2015-07-07T14:45:19Z","abstract_excerpt":"We investigate even-even two-proton borromean systems at prominent intermediate heavy waiting points for the rapid proton capture process. The most likely single-particle levels are used to calculate three-body energy and structure as a function of proton-core resonance energy. We establish a linear dependence between two- and three-body energies with the same slope, but the absolute value slightly dependent on partial wave structure. Using these relations we predict low-lying excited states in the isotones following the critical waiting points. The capture rate for producing a borromean bound"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.01828","kind":"arxiv","version":3},"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":"1507.01828","created_at":"2026-05-18T01:21:31.912889+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.01828v3","created_at":"2026-05-18T01:21:31.912889+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.01828","created_at":"2026-05-18T01:21:31.912889+00:00"},{"alias_kind":"pith_short_12","alias_value":"M7TBGALBC6LQ","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_16","alias_value":"M7TBGALBC6LQ3RM2","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_8","alias_value":"M7TBGALB","created_at":"2026-05-18T12:29:32.376354+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1907.11013","citing_title":"Studies of quasiclassical approach applicability to true three-body decays","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ","json":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ.json","graph_json":"https://pith.science/api/pith-number/M7TBGALBC6LQ3RM2DY6FB7SILZ/graph.json","events_json":"https://pith.science/api/pith-number/M7TBGALBC6LQ3RM2DY6FB7SILZ/events.json","paper":"https://pith.science/paper/M7TBGALB"},"agent_actions":{"view_html":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ","download_json":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ.json","view_paper":"https://pith.science/paper/M7TBGALB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.01828&json=true","fetch_graph":"https://pith.science/api/pith-number/M7TBGALBC6LQ3RM2DY6FB7SILZ/graph.json","fetch_events":"https://pith.science/api/pith-number/M7TBGALBC6LQ3RM2DY6FB7SILZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ/action/storage_attestation","attest_author":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ/action/author_attestation","sign_citation":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ/action/citation_signature","submit_replication":"https://pith.science/pith/M7TBGALBC6LQ3RM2DY6FB7SILZ/action/replication_record"}},"created_at":"2026-05-18T01:21:31.912889+00:00","updated_at":"2026-05-18T01:21:31.912889+00:00"}