{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:UDTOIY5G7O7W5SSYR2B5NEIWMB","short_pith_number":"pith:UDTOIY5G","schema_version":"1.0","canonical_sha256":"a0e6e463a6fbbf6eca588e83d69116606b15b2b62872bfa57fcee295bb7c8427","source":{"kind":"arxiv","id":"nucl-th/0203013","version":3},"attestation_state":"computed","paper":{"title":"Ab initio approach to s-shell hypernuclei 3H_Lambda, 4H_Lambda, 4He_Lambda and 5He_Lambda with a Lambda N-Sigma N interaction","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Nemura, Y. Akaishi, Y. Suzuki","submitted_at":"2002-03-08T15:15:14Z","abstract_excerpt":"Variational calculations for s-shell hypernuclei are performed by explicitly including $\\Sigma$ degrees of freedom. Four sets of YN interactions (SC97d(S), SC97e(S), SC97f(S) and SC89(S)) are used. The bound-state solution of $_\\Lambda^5$He is obtained and a large energy expectation value of the tensor $\\Lambda N-\\Sigma N$ transition part is found. The internal energy of the $^4$He subsystem is strongly affected by the presence of a $\\Lambda$ particle with the strong tensor $\\Lambda N-\\Sigma N$ transition potential."},"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":"nucl-th/0203013","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2002-03-08T15:15:14Z","cross_cats_sorted":[],"title_canon_sha256":"ea2e32a9898d5147a4a7298544b40b30bd7cf35225bbe482fa075ea55370993d","abstract_canon_sha256":"05cd3daa666cf9fc2d5fb5b6d3f78eff3d5f67dfcab2aaab815b160544e8c422"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:35:26.229904Z","signature_b64":"mn9k01cvr4vzFun1rVmBk4d1vAl8bKfPiHQ5Xusihz+kcJ6g+5ExEIxaFYijDiKTIVwOFvxSt/PN4xQK2v0kDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0e6e463a6fbbf6eca588e83d69116606b15b2b62872bfa57fcee295bb7c8427","last_reissued_at":"2026-07-04T16:35:26.229550Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:35:26.229550Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ab initio approach to s-shell hypernuclei 3H_Lambda, 4H_Lambda, 4He_Lambda and 5He_Lambda with a Lambda N-Sigma N interaction","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Nemura, Y. Akaishi, Y. Suzuki","submitted_at":"2002-03-08T15:15:14Z","abstract_excerpt":"Variational calculations for s-shell hypernuclei are performed by explicitly including $\\Sigma$ degrees of freedom. Four sets of YN interactions (SC97d(S), SC97e(S), SC97f(S) and SC89(S)) are used. The bound-state solution of $_\\Lambda^5$He is obtained and a large energy expectation value of the tensor $\\Lambda N-\\Sigma N$ transition part is found. The internal energy of the $^4$He subsystem is strongly affected by the presence of a $\\Lambda$ particle with the strong tensor $\\Lambda N-\\Sigma N$ transition potential."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0203013","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/0203013/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":"nucl-th/0203013","created_at":"2026-07-04T16:35:26.229610+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0203013v3","created_at":"2026-07-04T16:35:26.229610+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0203013","created_at":"2026-07-04T16:35:26.229610+00:00"},{"alias_kind":"pith_short_12","alias_value":"UDTOIY5G7O7W","created_at":"2026-07-04T16:35:26.229610+00:00"},{"alias_kind":"pith_short_16","alias_value":"UDTOIY5G7O7W5SSY","created_at":"2026-07-04T16:35:26.229610+00:00"},{"alias_kind":"pith_short_8","alias_value":"UDTOIY5G","created_at":"2026-07-04T16:35:26.229610+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.16994","citing_title":"Hypernuclei with Neural Network Quantum States","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB","json":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB.json","graph_json":"https://pith.science/api/pith-number/UDTOIY5G7O7W5SSYR2B5NEIWMB/graph.json","events_json":"https://pith.science/api/pith-number/UDTOIY5G7O7W5SSYR2B5NEIWMB/events.json","paper":"https://pith.science/paper/UDTOIY5G"},"agent_actions":{"view_html":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB","download_json":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB.json","view_paper":"https://pith.science/paper/UDTOIY5G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0203013&json=true","fetch_graph":"https://pith.science/api/pith-number/UDTOIY5G7O7W5SSYR2B5NEIWMB/graph.json","fetch_events":"https://pith.science/api/pith-number/UDTOIY5G7O7W5SSYR2B5NEIWMB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB/action/storage_attestation","attest_author":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB/action/author_attestation","sign_citation":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB/action/citation_signature","submit_replication":"https://pith.science/pith/UDTOIY5G7O7W5SSYR2B5NEIWMB/action/replication_record"}},"created_at":"2026-07-04T16:35:26.229610+00:00","updated_at":"2026-07-04T16:35:26.229610+00:00"}