{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:UIHKEGH35UT4VI27JVDLXGGMMS","short_pith_number":"pith:UIHKEGH3","schema_version":"1.0","canonical_sha256":"a20ea218fbed27caa35f4d46bb98cc64a79b6466f0dfc58151ee24ec3fa431d6","source":{"kind":"arxiv","id":"1705.03446","version":1},"attestation_state":"computed","paper":{"title":"Faddeev calculations for light $\\Xi$-hypernuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Branislav Vlahovic, Igor Filikhin, Vladimir M. Suslov","submitted_at":"2017-05-09T17:49:19Z","abstract_excerpt":"The hypernuclear systems $NN\\Xi $ and $\\Xi\\Xi N$ are considered as an analogue of $nnp$ ($^3$H) nuclear system (with the notation as $AAB$ system). We use the recently proposed modification for the $s$-wave Malfliet-Tjon potential. The modification simulates the Extended-Soft-Core model (ESC08c) for baryon-baryon interactions. The $\\Xi N$ spin/isospin triplet $(S, I)=(1, 1)$ potential generates a bound state with the energy $B_2(AB)$=1.56~MeV. Three-body binding energy $B_3$ for the states with maximal total isospin is calculated employing the configuration-space Faddeev equations. Comparison "},"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":"1705.03446","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-05-09T17:49:19Z","cross_cats_sorted":[],"title_canon_sha256":"e00f9773356c5f7635e44cab4af18b44dc4104ea67665e1e44e7ff057a504864","abstract_canon_sha256":"6ca108962042ce119dc2a2901a72daa93f95f26f03d7b908a8b13011350a2dbe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:47.827368Z","signature_b64":"tzt3R4uiyakgJ02SFg0igpWYZmv4XyTf10RyNDArGf/DWX9t3B/B6khBd+BosgydFYjAzBwq1oEvm7U2bhYMAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a20ea218fbed27caa35f4d46bb98cc64a79b6466f0dfc58151ee24ec3fa431d6","last_reissued_at":"2026-05-18T00:44:47.826952Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:47.826952Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Faddeev calculations for light $\\Xi$-hypernuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Branislav Vlahovic, Igor Filikhin, Vladimir M. Suslov","submitted_at":"2017-05-09T17:49:19Z","abstract_excerpt":"The hypernuclear systems $NN\\Xi $ and $\\Xi\\Xi N$ are considered as an analogue of $nnp$ ($^3$H) nuclear system (with the notation as $AAB$ system). We use the recently proposed modification for the $s$-wave Malfliet-Tjon potential. The modification simulates the Extended-Soft-Core model (ESC08c) for baryon-baryon interactions. The $\\Xi N$ spin/isospin triplet $(S, I)=(1, 1)$ potential generates a bound state with the energy $B_2(AB)$=1.56~MeV. Three-body binding energy $B_3$ for the states with maximal total isospin is calculated employing the configuration-space Faddeev equations. Comparison "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.03446","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":""},"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":"1705.03446","created_at":"2026-05-18T00:44:47.827011+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.03446v1","created_at":"2026-05-18T00:44:47.827011+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.03446","created_at":"2026-05-18T00:44:47.827011+00:00"},{"alias_kind":"pith_short_12","alias_value":"UIHKEGH35UT4","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"UIHKEGH35UT4VI27","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"UIHKEGH3","created_at":"2026-05-18T12:31:46.661854+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/UIHKEGH35UT4VI27JVDLXGGMMS","json":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS.json","graph_json":"https://pith.science/api/pith-number/UIHKEGH35UT4VI27JVDLXGGMMS/graph.json","events_json":"https://pith.science/api/pith-number/UIHKEGH35UT4VI27JVDLXGGMMS/events.json","paper":"https://pith.science/paper/UIHKEGH3"},"agent_actions":{"view_html":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS","download_json":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS.json","view_paper":"https://pith.science/paper/UIHKEGH3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.03446&json=true","fetch_graph":"https://pith.science/api/pith-number/UIHKEGH35UT4VI27JVDLXGGMMS/graph.json","fetch_events":"https://pith.science/api/pith-number/UIHKEGH35UT4VI27JVDLXGGMMS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS/action/storage_attestation","attest_author":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS/action/author_attestation","sign_citation":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS/action/citation_signature","submit_replication":"https://pith.science/pith/UIHKEGH35UT4VI27JVDLXGGMMS/action/replication_record"}},"created_at":"2026-05-18T00:44:47.827011+00:00","updated_at":"2026-05-18T00:44:47.827011+00:00"}