{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:SYGYYT3SN3UNHPGAMGAEWFQXBU","short_pith_number":"pith:SYGYYT3S","schema_version":"1.0","canonical_sha256":"960d8c4f726ee8d3bcc061804b16170d2c0dc66d27431d1940a1054e29958e0c","source":{"kind":"arxiv","id":"2110.12398","version":1},"attestation_state":"computed","paper":{"title":"A global study of $^9$Be + p at 2.72 A MeV","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. M. S\\'anchez-Ben\\'itez, A. Pakou, A. Spatafora, C. Agodi, D. Carbone, D. Torresi, F. Cappuzzello, G. A. Brischetto, G. Souliotis, I. Ciraldo, I. Dimitropoulos, I. Martel, J. Casal, L. La Fauci, M. Cavallaro, M. Rodr\\'iguez-Gallardo, O. Sgouros, S. Calabrese, S. Koulouris, V. Soukeras","submitted_at":"2021-10-24T09:37:22Z","abstract_excerpt":"Background: In our recent experiment, $^9$Be+p at 5.67A MeV, the breakup decay rates to the 3 configurations, $\\alpha$+$\\alpha$+n, $^8$Be$^*$+n and $^5$He+$^4$He of $^9$Be, were observed and quantified, in a full kinematics approach. Unfolding step by step the accessibility to the above configurations, it will require similar studies at lower and higher energies as well as the interpretation of the data in a theoretical framework. Purpose: Investigate the breakup decay rate of $^9$Be+p at 2.72A MeV, where the $\\alpha$+$\\alpha$+n configuration is mainly accessible. Compare and interpret data at"},"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":"2110.12398","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"nucl-ex","submitted_at":"2021-10-24T09:37:22Z","cross_cats_sorted":[],"title_canon_sha256":"f2ec0fb0c6875d8f734d09d19cf9de793854a89a46873d5267d07e20785bdfae","abstract_canon_sha256":"4a887867101bfdee70b0ed54ea839df50017660d310bd15608f330675b96e4c1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:25:19.969599Z","signature_b64":"QV8krPdRGsRLLsnkvIz499+y/26stLPV8JSFnGbnKaICY4+yVuT69tkU/gCvNqyTMwQuZvdCEnhXvi2TWuX0CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"960d8c4f726ee8d3bcc061804b16170d2c0dc66d27431d1940a1054e29958e0c","last_reissued_at":"2026-07-05T03:25:19.969123Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:25:19.969123Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A global study of $^9$Be + p at 2.72 A MeV","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. M. S\\'anchez-Ben\\'itez, A. Pakou, A. Spatafora, C. Agodi, D. Carbone, D. Torresi, F. Cappuzzello, G. A. Brischetto, G. Souliotis, I. Ciraldo, I. Dimitropoulos, I. Martel, J. Casal, L. La Fauci, M. Cavallaro, M. Rodr\\'iguez-Gallardo, O. Sgouros, S. Calabrese, S. Koulouris, V. Soukeras","submitted_at":"2021-10-24T09:37:22Z","abstract_excerpt":"Background: In our recent experiment, $^9$Be+p at 5.67A MeV, the breakup decay rates to the 3 configurations, $\\alpha$+$\\alpha$+n, $^8$Be$^*$+n and $^5$He+$^4$He of $^9$Be, were observed and quantified, in a full kinematics approach. Unfolding step by step the accessibility to the above configurations, it will require similar studies at lower and higher energies as well as the interpretation of the data in a theoretical framework. Purpose: Investigate the breakup decay rate of $^9$Be+p at 2.72A MeV, where the $\\alpha$+$\\alpha$+n configuration is mainly accessible. Compare and interpret data at"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.12398","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/2110.12398/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":"2110.12398","created_at":"2026-07-05T03:25:19.969184+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.12398v1","created_at":"2026-07-05T03:25:19.969184+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.12398","created_at":"2026-07-05T03:25:19.969184+00:00"},{"alias_kind":"pith_short_12","alias_value":"SYGYYT3SN3UN","created_at":"2026-07-05T03:25:19.969184+00:00"},{"alias_kind":"pith_short_16","alias_value":"SYGYYT3SN3UNHPGA","created_at":"2026-07-05T03:25:19.969184+00:00"},{"alias_kind":"pith_short_8","alias_value":"SYGYYT3S","created_at":"2026-07-05T03:25:19.969184+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/SYGYYT3SN3UNHPGAMGAEWFQXBU","json":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU.json","graph_json":"https://pith.science/api/pith-number/SYGYYT3SN3UNHPGAMGAEWFQXBU/graph.json","events_json":"https://pith.science/api/pith-number/SYGYYT3SN3UNHPGAMGAEWFQXBU/events.json","paper":"https://pith.science/paper/SYGYYT3S"},"agent_actions":{"view_html":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU","download_json":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU.json","view_paper":"https://pith.science/paper/SYGYYT3S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.12398&json=true","fetch_graph":"https://pith.science/api/pith-number/SYGYYT3SN3UNHPGAMGAEWFQXBU/graph.json","fetch_events":"https://pith.science/api/pith-number/SYGYYT3SN3UNHPGAMGAEWFQXBU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU/action/storage_attestation","attest_author":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU/action/author_attestation","sign_citation":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU/action/citation_signature","submit_replication":"https://pith.science/pith/SYGYYT3SN3UNHPGAMGAEWFQXBU/action/replication_record"}},"created_at":"2026-07-05T03:25:19.969184+00:00","updated_at":"2026-07-05T03:25:19.969184+00:00"}