{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JXEOBO5E63LSJRUQESJIJPSJ2P","short_pith_number":"pith:JXEOBO5E","schema_version":"1.0","canonical_sha256":"4dc8e0bba4f6d724c690249284be49d3d34b9f758bfe5457547c4aa242c2840f","source":{"kind":"arxiv","id":"2405.02892","version":1},"attestation_state":"computed","paper":{"title":"Study of the $^7$Be($d$,$^3$He)$^6$Li* reaction at 5 MeV/u","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. M. Moro, A. Perea, D. Gupta, I. Martel, J. Cederkall, J.D. Ovejas, J. Park, K. Kundalia, O. Tengblad, Sk M. Ali, S. Maity, Swapan K Saha","submitted_at":"2024-05-05T11:10:03Z","abstract_excerpt":"The measurement of the $^7$Be($d$,$^3$He)$^6$Li* transfer cross section at 5 MeV/u is carried out. The population of the 2.186 MeV excited state of $^6$Li in this reaction channel is observed for the first time. The experimental angular distributions have been analyzed in the finite range DWBA and coupled-channel frameworks. The effect of the $^7$Be($d$,$^3$He)$^6$Li reaction on both the $^6$Li and $^7$Li abundances are investigated at the relevant big-bang nucleosynthesis energies. The excitation function is calculated by TALYS and normalized to the experimental data. The $S$ factor of the ($"},"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":"2405.02892","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2024-05-05T11:10:03Z","cross_cats_sorted":[],"title_canon_sha256":"26bd73838162b57b8eece2619a1d4f607c26f666cd9f65506bab5315c4bae498","abstract_canon_sha256":"592caa402dd186728e6b01e6e7532929b521d0f1c1d6c95b9df69463e0ab56f7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:15:55.501932Z","signature_b64":"e4/FOu4s7wxu3ufh1cYcA7TaY8dWDEkuqHUrab9oi2gMkz9Uh+9c8jZpcNPapOZTXxlp8JmOWhMQANYGBssUCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4dc8e0bba4f6d724c690249284be49d3d34b9f758bfe5457547c4aa242c2840f","last_reissued_at":"2026-07-05T08:15:55.501383Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:15:55.501383Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Study of the $^7$Be($d$,$^3$He)$^6$Li* reaction at 5 MeV/u","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. M. Moro, A. Perea, D. Gupta, I. Martel, J. Cederkall, J.D. Ovejas, J. Park, K. Kundalia, O. Tengblad, Sk M. Ali, S. Maity, Swapan K Saha","submitted_at":"2024-05-05T11:10:03Z","abstract_excerpt":"The measurement of the $^7$Be($d$,$^3$He)$^6$Li* transfer cross section at 5 MeV/u is carried out. The population of the 2.186 MeV excited state of $^6$Li in this reaction channel is observed for the first time. The experimental angular distributions have been analyzed in the finite range DWBA and coupled-channel frameworks. The effect of the $^7$Be($d$,$^3$He)$^6$Li reaction on both the $^6$Li and $^7$Li abundances are investigated at the relevant big-bang nucleosynthesis energies. The excitation function is calculated by TALYS and normalized to the experimental data. The $S$ factor of the ($"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.02892","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/2405.02892/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":"2405.02892","created_at":"2026-07-05T08:15:55.501436+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.02892v1","created_at":"2026-07-05T08:15:55.501436+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.02892","created_at":"2026-07-05T08:15:55.501436+00:00"},{"alias_kind":"pith_short_12","alias_value":"JXEOBO5E63LS","created_at":"2026-07-05T08:15:55.501436+00:00"},{"alias_kind":"pith_short_16","alias_value":"JXEOBO5E63LSJRUQ","created_at":"2026-07-05T08:15:55.501436+00:00"},{"alias_kind":"pith_short_8","alias_value":"JXEOBO5E","created_at":"2026-07-05T08:15:55.501436+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/JXEOBO5E63LSJRUQESJIJPSJ2P","json":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P.json","graph_json":"https://pith.science/api/pith-number/JXEOBO5E63LSJRUQESJIJPSJ2P/graph.json","events_json":"https://pith.science/api/pith-number/JXEOBO5E63LSJRUQESJIJPSJ2P/events.json","paper":"https://pith.science/paper/JXEOBO5E"},"agent_actions":{"view_html":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P","download_json":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P.json","view_paper":"https://pith.science/paper/JXEOBO5E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.02892&json=true","fetch_graph":"https://pith.science/api/pith-number/JXEOBO5E63LSJRUQESJIJPSJ2P/graph.json","fetch_events":"https://pith.science/api/pith-number/JXEOBO5E63LSJRUQESJIJPSJ2P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P/action/storage_attestation","attest_author":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P/action/author_attestation","sign_citation":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P/action/citation_signature","submit_replication":"https://pith.science/pith/JXEOBO5E63LSJRUQESJIJPSJ2P/action/replication_record"}},"created_at":"2026-07-05T08:15:55.501436+00:00","updated_at":"2026-07-05T08:15:55.501436+00:00"}