{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:HLR32C5IWS533DGQOD3GBSH6IG","short_pith_number":"pith:HLR32C5I","schema_version":"1.0","canonical_sha256":"3ae3bd0ba8b4bbbd8cd070f660c8fe41a1ffdaec94c97698f7675d81534be84e","source":{"kind":"arxiv","id":"hep-ph/0507071","version":2},"attestation_state":"computed","paper":{"title":"Coupled-channel study of crypto-exotic baryons with charm","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"J. Hofmann, M.F.M. Lutz (GSI)","submitted_at":"2005-07-06T13:33:59Z","abstract_excerpt":"Identifying the t-channel exchange of vector mesons as the driving force for the s-wave scattering of pseudo-scalar mesons off the baryon ground states, a surprisingly rich spectrum of molecules is formed. We argue that chiral symmetry and large- N_c considerations determine that part of the interaction which generates the spectrum. All channels that are required by the existence of (u,d,s,c) quarks are considered. A bound state with exotic quantum numbers is predicted at mass 2.78 GeV. It couples strongly to the (bar D_s N),(bar D Lambda),(bar D Sigma) channels. A further charm minus-one syst"},"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":"hep-ph/0507071","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-07-06T13:33:59Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"de9975758de3230ea2d883c781d369b6778f745ca2b8e33cf2ef0a8c949edc94","abstract_canon_sha256":"f2d32dfc4db3b40288507fea504c14fb4f4fbad33dd70cd1fe3fa543245d6989"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:33:16.623055Z","signature_b64":"UIOWvqQpyA+2i8HZqht2s0/n76JWpGTIzRp60htjbsj3MiHOjveO4sAvsbPnP4NMqt37Hjb7jUzEehDEw+y9CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ae3bd0ba8b4bbbd8cd070f660c8fe41a1ffdaec94c97698f7675d81534be84e","last_reissued_at":"2026-05-18T04:33:16.622521Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:33:16.622521Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coupled-channel study of crypto-exotic baryons with charm","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"J. Hofmann, M.F.M. Lutz (GSI)","submitted_at":"2005-07-06T13:33:59Z","abstract_excerpt":"Identifying the t-channel exchange of vector mesons as the driving force for the s-wave scattering of pseudo-scalar mesons off the baryon ground states, a surprisingly rich spectrum of molecules is formed. We argue that chiral symmetry and large- N_c considerations determine that part of the interaction which generates the spectrum. All channels that are required by the existence of (u,d,s,c) quarks are considered. A bound state with exotic quantum numbers is predicted at mass 2.78 GeV. It couples strongly to the (bar D_s N),(bar D Lambda),(bar D Sigma) channels. A further charm minus-one syst"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0507071","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":""},"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":"hep-ph/0507071","created_at":"2026-05-18T04:33:16.622598+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0507071v2","created_at":"2026-05-18T04:33:16.622598+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0507071","created_at":"2026-05-18T04:33:16.622598+00:00"},{"alias_kind":"pith_short_12","alias_value":"HLR32C5IWS53","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"HLR32C5IWS533DGQ","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"HLR32C5I","created_at":"2026-05-18T12:25:53.335082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.21205","citing_title":"Comprehensive study of hidden charm pentaquarks with an improved unitarization method","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2603.02979","citing_title":"Scattering and Femtoscopic Correlation Functions of the $\\Sigma_c^{++}\\pi^{+}$, $\\Sigma_c^{0}\\pi^{-}$ and $\\Sigma_b^{+}\\pi^{+}$ Systems","ref_index":49,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG","json":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG.json","graph_json":"https://pith.science/api/pith-number/HLR32C5IWS533DGQOD3GBSH6IG/graph.json","events_json":"https://pith.science/api/pith-number/HLR32C5IWS533DGQOD3GBSH6IG/events.json","paper":"https://pith.science/paper/HLR32C5I"},"agent_actions":{"view_html":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG","download_json":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG.json","view_paper":"https://pith.science/paper/HLR32C5I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0507071&json=true","fetch_graph":"https://pith.science/api/pith-number/HLR32C5IWS533DGQOD3GBSH6IG/graph.json","fetch_events":"https://pith.science/api/pith-number/HLR32C5IWS533DGQOD3GBSH6IG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG/action/storage_attestation","attest_author":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG/action/author_attestation","sign_citation":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG/action/citation_signature","submit_replication":"https://pith.science/pith/HLR32C5IWS533DGQOD3GBSH6IG/action/replication_record"}},"created_at":"2026-05-18T04:33:16.622598+00:00","updated_at":"2026-05-18T04:33:16.622598+00:00"}