{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ISTRBWD3RJTX6VZ4G72CHNO55E","short_pith_number":"pith:ISTRBWD3","schema_version":"1.0","canonical_sha256":"44a710d87b8a677f573c37f423b5dde939810d1050fb2dda131ed84327d89dfb","source":{"kind":"arxiv","id":"2404.04016","version":1},"attestation_state":"computed","paper":{"title":"Flavor-spin symmetry of the $P^N_{\\psi}/H_{\\Omega_{ccc}}^N$ and $P^\\Lambda_{\\psi s}/H^{\\Lambda}_{\\Omega_{ccc}s}$ molecular states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bo Wang, Kan Chen","submitted_at":"2024-04-05T10:58:17Z","abstract_excerpt":"Based on a contact lagrangian that incorporates the SU(3) flavor and SU(2) spin symmetries, we discuss the symmetry properties of the interactions among the heavy flavor meson-baryon $P_{\\psi}^N$, $P_{\\psi s}^\\Lambda$ (with quark components [$n\\bar{c}$][$nnc$], [$s\\bar{c}$][$nnc$], or [$n\\bar{c}$][$nsc$]) systems and di-baryon $H_{\\Omega_{ccc}}^N$, $H^{\\Lambda}_{\\Omega_{ccc}s}$ (with quark components [$nnc$][$ncc$], [$nnc$][$scc$] or [$nsc$][$ncc$]) systems ($n=u$, $d$). The light quark components of the $P_{\\psi}^N$ ($P_{\\psi s}^\\Lambda$) and $H_{\\Omega_{ccc}}^N$ ($H_{\\Omega_{ccc}s}^\\Lambda$)"},"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":"2404.04016","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-05T10:58:17Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"fd2d0f034b757fa4612c660523aa6d77288cd6351ea0b19088e60b1cbf7454c4","abstract_canon_sha256":"86055038430e28a4d9810de4d2b48b81d095a22c5cdd5a6d43dc10605624e353"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:04:44.424904Z","signature_b64":"C8IOqvGAMGafz6BARo+9EjrTCBzcur5EIYU53CMfKa+iW9H+WVYdFnssNU9YPZ0XOXafkYeW+Fx/HMvP3hQxAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"44a710d87b8a677f573c37f423b5dde939810d1050fb2dda131ed84327d89dfb","last_reissued_at":"2026-07-05T08:04:44.424428Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:04:44.424428Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Flavor-spin symmetry of the $P^N_{\\psi}/H_{\\Omega_{ccc}}^N$ and $P^\\Lambda_{\\psi s}/H^{\\Lambda}_{\\Omega_{ccc}s}$ molecular states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bo Wang, Kan Chen","submitted_at":"2024-04-05T10:58:17Z","abstract_excerpt":"Based on a contact lagrangian that incorporates the SU(3) flavor and SU(2) spin symmetries, we discuss the symmetry properties of the interactions among the heavy flavor meson-baryon $P_{\\psi}^N$, $P_{\\psi s}^\\Lambda$ (with quark components [$n\\bar{c}$][$nnc$], [$s\\bar{c}$][$nnc$], or [$n\\bar{c}$][$nsc$]) systems and di-baryon $H_{\\Omega_{ccc}}^N$, $H^{\\Lambda}_{\\Omega_{ccc}s}$ (with quark components [$nnc$][$ncc$], [$nnc$][$scc$] or [$nsc$][$ncc$]) systems ($n=u$, $d$). The light quark components of the $P_{\\psi}^N$ ($P_{\\psi s}^\\Lambda$) and $H_{\\Omega_{ccc}}^N$ ($H_{\\Omega_{ccc}s}^\\Lambda$)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.04016","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/2404.04016/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":"2404.04016","created_at":"2026-07-05T08:04:44.424486+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.04016v1","created_at":"2026-07-05T08:04:44.424486+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.04016","created_at":"2026-07-05T08:04:44.424486+00:00"},{"alias_kind":"pith_short_12","alias_value":"ISTRBWD3RJTX","created_at":"2026-07-05T08:04:44.424486+00:00"},{"alias_kind":"pith_short_16","alias_value":"ISTRBWD3RJTX6VZ4","created_at":"2026-07-05T08:04:44.424486+00:00"},{"alias_kind":"pith_short_8","alias_value":"ISTRBWD3","created_at":"2026-07-05T08:04:44.424486+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.10318","citing_title":"Electromagnetic properties of possible triple-charm molecular hexaquarks","ref_index":36,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E","json":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E.json","graph_json":"https://pith.science/api/pith-number/ISTRBWD3RJTX6VZ4G72CHNO55E/graph.json","events_json":"https://pith.science/api/pith-number/ISTRBWD3RJTX6VZ4G72CHNO55E/events.json","paper":"https://pith.science/paper/ISTRBWD3"},"agent_actions":{"view_html":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E","download_json":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E.json","view_paper":"https://pith.science/paper/ISTRBWD3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.04016&json=true","fetch_graph":"https://pith.science/api/pith-number/ISTRBWD3RJTX6VZ4G72CHNO55E/graph.json","fetch_events":"https://pith.science/api/pith-number/ISTRBWD3RJTX6VZ4G72CHNO55E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E/action/storage_attestation","attest_author":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E/action/author_attestation","sign_citation":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E/action/citation_signature","submit_replication":"https://pith.science/pith/ISTRBWD3RJTX6VZ4G72CHNO55E/action/replication_record"}},"created_at":"2026-07-05T08:04:44.424486+00:00","updated_at":"2026-07-05T08:04:44.424486+00:00"}