{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:GUBVFFKJRUBQSK6G6WSKI7RAO7","short_pith_number":"pith:GUBVFFKJ","schema_version":"1.0","canonical_sha256":"35035295498d03092bc6f5a4a47e2077ffc7898c2e897de961196fef7de44fea","source":{"kind":"arxiv","id":"2503.04264","version":2},"attestation_state":"computed","paper":{"title":"Towards modeling the short-range interactions of hidden/open charm pentaquark molecular states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Hai-Xiang Zhu, Lu Meng, Ning Li, Ru Xu, Wei Chen","submitted_at":"2025-03-06T09:48:46Z","abstract_excerpt":"The hadronic $\\Sigma_c^{(*)}\\bar{D}^{(*)}$ and $\\Sigma_c^{(*)}{D}^{(*)}$ interactions are revisited, with a focus on their short-range parts, motivated by a tension between the interpretations of $P_{c\\bar{c}}(4312)$, $P_{c\\bar{c}}(4440)$, and $P_{c\\bar{c}}(4457)$ in effective field theory (EFT) frameworks and the one-boson-exchange (OBE) model. While the three states can be interpreted as $\\Sigma_c\\bar{D}^{(*)}$ molecular states within EFT frameworks, this is not feasible in the single-channel OBE model with consistent cutoff. In this work, the possibility to reconcile OBE model with EFTs by "},"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":"2503.04264","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-03-06T09:48:46Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"91ccb0796c3d5d6908ea1756f412cff217fa2ef99cf4f54ad2d1df6e37497fe8","abstract_canon_sha256":"98cd5c6dd9a3ca831d5d3b1339f06d963f154a26071e27e0dc97a16bbc640aba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:01:32.586173Z","signature_b64":"rykQwedwiuDlBQRVmkLvacwI32Kib0yTiNBa3XLCrs/ecodFLN/oF0W7Reb11fQQVCTB/B+jQxMrqyH6a89mBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"35035295498d03092bc6f5a4a47e2077ffc7898c2e897de961196fef7de44fea","last_reissued_at":"2026-07-05T11:01:32.585621Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:01:32.585621Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Towards modeling the short-range interactions of hidden/open charm pentaquark molecular states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Hai-Xiang Zhu, Lu Meng, Ning Li, Ru Xu, Wei Chen","submitted_at":"2025-03-06T09:48:46Z","abstract_excerpt":"The hadronic $\\Sigma_c^{(*)}\\bar{D}^{(*)}$ and $\\Sigma_c^{(*)}{D}^{(*)}$ interactions are revisited, with a focus on their short-range parts, motivated by a tension between the interpretations of $P_{c\\bar{c}}(4312)$, $P_{c\\bar{c}}(4440)$, and $P_{c\\bar{c}}(4457)$ in effective field theory (EFT) frameworks and the one-boson-exchange (OBE) model. While the three states can be interpreted as $\\Sigma_c\\bar{D}^{(*)}$ molecular states within EFT frameworks, this is not feasible in the single-channel OBE model with consistent cutoff. In this work, the possibility to reconcile OBE model with EFTs by "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.04264","kind":"arxiv","version":2},"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/2503.04264/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":"2503.04264","created_at":"2026-07-05T11:01:32.585682+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.04264v2","created_at":"2026-07-05T11:01:32.585682+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.04264","created_at":"2026-07-05T11:01:32.585682+00:00"},{"alias_kind":"pith_short_12","alias_value":"GUBVFFKJRUBQ","created_at":"2026-07-05T11:01:32.585682+00:00"},{"alias_kind":"pith_short_16","alias_value":"GUBVFFKJRUBQSK6G","created_at":"2026-07-05T11:01:32.585682+00:00"},{"alias_kind":"pith_short_8","alias_value":"GUBVFFKJ","created_at":"2026-07-05T11:01:32.585682+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.23298","citing_title":"Coupled-channel study of the three-body $DDK$ and $D^{*}D^{*}K$","ref_index":75,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7","json":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7.json","graph_json":"https://pith.science/api/pith-number/GUBVFFKJRUBQSK6G6WSKI7RAO7/graph.json","events_json":"https://pith.science/api/pith-number/GUBVFFKJRUBQSK6G6WSKI7RAO7/events.json","paper":"https://pith.science/paper/GUBVFFKJ"},"agent_actions":{"view_html":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7","download_json":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7.json","view_paper":"https://pith.science/paper/GUBVFFKJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.04264&json=true","fetch_graph":"https://pith.science/api/pith-number/GUBVFFKJRUBQSK6G6WSKI7RAO7/graph.json","fetch_events":"https://pith.science/api/pith-number/GUBVFFKJRUBQSK6G6WSKI7RAO7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7/action/storage_attestation","attest_author":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7/action/author_attestation","sign_citation":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7/action/citation_signature","submit_replication":"https://pith.science/pith/GUBVFFKJRUBQSK6G6WSKI7RAO7/action/replication_record"}},"created_at":"2026-07-05T11:01:32.585682+00:00","updated_at":"2026-07-05T11:01:32.585682+00:00"}