{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:7RGV7GN333M34RZ6AO4ANOMNEN","short_pith_number":"pith:7RGV7GN3","schema_version":"1.0","canonical_sha256":"fc4d5f99bbded9be473e03b806b98d23773fea0402de011c2a7b1b868525996b","source":{"kind":"arxiv","id":"hep-lat/0305008","version":2},"attestation_state":"computed","paper":{"title":"Hybrid configuration content of heavy S-wave mesons","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Doug Toussaint, Tommy Burch","submitted_at":"2003-05-08T08:06:59Z","abstract_excerpt":"We use the non-relativistic expansion of QCD (NRQCD) on the lattice to study the lowest hybrid configuration contribution to the ground state of heavy S-wave mesons. Using lowest-order lattice NRQCD to create the heavy-quark propagators, we form a basis of ``unperturbed'' S-wave and hybrid states. We then apply the lowest-order coupling of the quark spin and chromomagnetic field at an intermediate time slice to create ``mixed'' correlators between the S-wave and hybrid states. From the resulting amplitudes, we extract the off-diagonal element of our two-state Hamiltonian. Diagonalizing this Ha"},"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-lat/0305008","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2003-05-08T08:06:59Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"dc3483ec729db916b1ac55260aab667aba52edd25fd16151b84ec7489791a42f","abstract_canon_sha256":"bb8cd0365ff0403342817dfdd5ef479d05343e48bbcc3325a8a503a1aae48558"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:17:38.822588Z","signature_b64":"EPZR+OgOujYZEa04HO/2Og8P9o8NAhsZ4UChHkTL4NLFSkb9ezCcInvEVTuW6N7Ax4wVKUOcGqoy2LYI00b6BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc4d5f99bbded9be473e03b806b98d23773fea0402de011c2a7b1b868525996b","last_reissued_at":"2026-07-04T15:17:38.822210Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:17:38.822210Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hybrid configuration content of heavy S-wave mesons","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Doug Toussaint, Tommy Burch","submitted_at":"2003-05-08T08:06:59Z","abstract_excerpt":"We use the non-relativistic expansion of QCD (NRQCD) on the lattice to study the lowest hybrid configuration contribution to the ground state of heavy S-wave mesons. Using lowest-order lattice NRQCD to create the heavy-quark propagators, we form a basis of ``unperturbed'' S-wave and hybrid states. We then apply the lowest-order coupling of the quark spin and chromomagnetic field at an intermediate time slice to create ``mixed'' correlators between the S-wave and hybrid states. From the resulting amplitudes, we extract the off-diagonal element of our two-state Hamiltonian. Diagonalizing this Ha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0305008","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/hep-lat/0305008/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":"hep-lat/0305008","created_at":"2026-07-04T15:17:38.822276+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0305008v2","created_at":"2026-07-04T15:17:38.822276+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0305008","created_at":"2026-07-04T15:17:38.822276+00:00"},{"alias_kind":"pith_short_12","alias_value":"7RGV7GN333M3","created_at":"2026-07-04T15:17:38.822276+00:00"},{"alias_kind":"pith_short_16","alias_value":"7RGV7GN333M34RZ6","created_at":"2026-07-04T15:17:38.822276+00:00"},{"alias_kind":"pith_short_8","alias_value":"7RGV7GN3","created_at":"2026-07-04T15:17:38.822276+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.08844","citing_title":"Hybrid spin-dependent and hybrid-quarkonium mixing potentials at order $(1 /m_Q)^1$ from SU(3) lattice gauge theory","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN","json":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN.json","graph_json":"https://pith.science/api/pith-number/7RGV7GN333M34RZ6AO4ANOMNEN/graph.json","events_json":"https://pith.science/api/pith-number/7RGV7GN333M34RZ6AO4ANOMNEN/events.json","paper":"https://pith.science/paper/7RGV7GN3"},"agent_actions":{"view_html":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN","download_json":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN.json","view_paper":"https://pith.science/paper/7RGV7GN3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0305008&json=true","fetch_graph":"https://pith.science/api/pith-number/7RGV7GN333M34RZ6AO4ANOMNEN/graph.json","fetch_events":"https://pith.science/api/pith-number/7RGV7GN333M34RZ6AO4ANOMNEN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN/action/storage_attestation","attest_author":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN/action/author_attestation","sign_citation":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN/action/citation_signature","submit_replication":"https://pith.science/pith/7RGV7GN333M34RZ6AO4ANOMNEN/action/replication_record"}},"created_at":"2026-07-04T15:17:38.822276+00:00","updated_at":"2026-07-04T15:17:38.822276+00:00"}