{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:HPXFIR6T2Q44HSJAYG655W7HZS","short_pith_number":"pith:HPXFIR6T","schema_version":"1.0","canonical_sha256":"3bee5447d3d439c3c920c1bddedbe7ccbdca0c1733b53662a991be05b7f748c6","source":{"kind":"arxiv","id":"2112.01823","version":4},"attestation_state":"computed","paper":{"title":"Magnetic moments of the hidden-charm strange pentaquark states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Feng Gao, Hao-Song Li","submitted_at":"2021-12-03T10:25:05Z","abstract_excerpt":"This paper calculates the magnetic moments of the hidden-charm strange pentaquark states with a quantum number of $J^P={\\frac{1}{2}}^{\\pm}$, ${\\frac{3}{2}}^{\\pm}$, ${\\frac{5}{2}}^{\\pm}$, and ${\\frac{7}{2}}^{+}$ in the molecular, diquark-diquark-antiquark, and diquark-triquark models, respectively. Numerical results demonstrate that the magnetic moments change for a different spin-orbit coupling with the same model and when involving different models with the same angular momentum."},"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":"2112.01823","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-12-03T10:25:05Z","cross_cats_sorted":[],"title_canon_sha256":"7abbed440a6b782968fbaa16d3ae4c9c9d195f01eb428a2c35c4f08785c74944","abstract_canon_sha256":"6bd2785a99256cc172275a16852a15eafbb81e7ce9effa8f41e2e78f95aaf197"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:22:42.321367Z","signature_b64":"Rv/2iv/1BRp1cXZwlzfCQNMtaDDfhGc2DCRCwcQVQpGFwRUiN0FgkurtamfO6rvliCLzmaZ64xKtlSSuaxa+Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3bee5447d3d439c3c920c1bddedbe7ccbdca0c1733b53662a991be05b7f748c6","last_reissued_at":"2026-07-05T05:22:42.320879Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:22:42.320879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic moments of the hidden-charm strange pentaquark states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Feng Gao, Hao-Song Li","submitted_at":"2021-12-03T10:25:05Z","abstract_excerpt":"This paper calculates the magnetic moments of the hidden-charm strange pentaquark states with a quantum number of $J^P={\\frac{1}{2}}^{\\pm}$, ${\\frac{3}{2}}^{\\pm}$, ${\\frac{5}{2}}^{\\pm}$, and ${\\frac{7}{2}}^{+}$ in the molecular, diquark-diquark-antiquark, and diquark-triquark models, respectively. Numerical results demonstrate that the magnetic moments change for a different spin-orbit coupling with the same model and when involving different models with the same angular momentum."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.01823","kind":"arxiv","version":4},"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/2112.01823/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":"2112.01823","created_at":"2026-07-05T05:22:42.320935+00:00"},{"alias_kind":"arxiv_version","alias_value":"2112.01823v4","created_at":"2026-07-05T05:22:42.320935+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.01823","created_at":"2026-07-05T05:22:42.320935+00:00"},{"alias_kind":"pith_short_12","alias_value":"HPXFIR6T2Q44","created_at":"2026-07-05T05:22:42.320935+00:00"},{"alias_kind":"pith_short_16","alias_value":"HPXFIR6T2Q44HSJA","created_at":"2026-07-05T05:22:42.320935+00:00"},{"alias_kind":"pith_short_8","alias_value":"HPXFIR6T","created_at":"2026-07-05T05:22:42.320935+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.04355","citing_title":"Charting doubly strange hidden-charm pentaquarks: An electromagnetic mapping of spin-$\\frac{1}{2}$ and $\\frac{3}{2}$ states","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS","json":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS.json","graph_json":"https://pith.science/api/pith-number/HPXFIR6T2Q44HSJAYG655W7HZS/graph.json","events_json":"https://pith.science/api/pith-number/HPXFIR6T2Q44HSJAYG655W7HZS/events.json","paper":"https://pith.science/paper/HPXFIR6T"},"agent_actions":{"view_html":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS","download_json":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS.json","view_paper":"https://pith.science/paper/HPXFIR6T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2112.01823&json=true","fetch_graph":"https://pith.science/api/pith-number/HPXFIR6T2Q44HSJAYG655W7HZS/graph.json","fetch_events":"https://pith.science/api/pith-number/HPXFIR6T2Q44HSJAYG655W7HZS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS/action/storage_attestation","attest_author":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS/action/author_attestation","sign_citation":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS/action/citation_signature","submit_replication":"https://pith.science/pith/HPXFIR6T2Q44HSJAYG655W7HZS/action/replication_record"}},"created_at":"2026-07-05T05:22:42.320935+00:00","updated_at":"2026-07-05T05:22:42.320935+00:00"}