{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:4LKR7QLNESJEEVXJFPKOPC6T2H","short_pith_number":"pith:4LKR7QLN","schema_version":"1.0","canonical_sha256":"e2d51fc16d24924256e92bd4e78bd3d1d4c564703d8bd14d1c8616eae46fcf5e","source":{"kind":"arxiv","id":"hep-lat/0512044","version":3},"attestation_state":"computed","paper":{"title":"Gluonic excitation of non-exotic hybrid charmonium from lattice QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Xiang-Qian Luo, Yan Liu (Zhongshan Univ.)","submitted_at":"2005-12-30T06:49:59Z","abstract_excerpt":"The ground and first excited states of the hybrid charmonium ${\\bar c} c g$, with non-exotic quantum numbers $J^{PC}=0^{-+}$, $1^{--}$ and $1^{++}$ are investigated using quenched lattice QCD. They are completely ignored in the literature, only because their ground states are degenerate with $\\eta_c$, $J/\\psi$, and $\\chi_{c1}$, and are difficult to be distinguished from these conventional charmonium mesons in experiment. However, we observe strong gluonic radial excitations in the first excited states; We predict that their masses are 4.352(225)GeV, 4.379(149)GeV and 7.315(257)GeV, completely "},"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/0512044","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-12-30T06:49:59Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a8852465f087cd0f285b5ad348c1e10d5154083f4dce7a7836d227f30850237f","abstract_canon_sha256":"790f8d87f1e89a87ba49448a4cdb5038fb58214cb44c2ff77c75e6937f735bc5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:20.098185Z","signature_b64":"aBE4nGzQCqCvE1+Q+AacD82rY6xsuCNNhn81Lw1FXwjVR3hbGjYtDnIzisoRmd8WE4wl7tStHRMavY2fkKpgCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e2d51fc16d24924256e92bd4e78bd3d1d4c564703d8bd14d1c8616eae46fcf5e","last_reissued_at":"2026-05-18T02:37:20.097775Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:20.097775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gluonic excitation of non-exotic hybrid charmonium from lattice QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Xiang-Qian Luo, Yan Liu (Zhongshan Univ.)","submitted_at":"2005-12-30T06:49:59Z","abstract_excerpt":"The ground and first excited states of the hybrid charmonium ${\\bar c} c g$, with non-exotic quantum numbers $J^{PC}=0^{-+}$, $1^{--}$ and $1^{++}$ are investigated using quenched lattice QCD. They are completely ignored in the literature, only because their ground states are degenerate with $\\eta_c$, $J/\\psi$, and $\\chi_{c1}$, and are difficult to be distinguished from these conventional charmonium mesons in experiment. However, we observe strong gluonic radial excitations in the first excited states; We predict that their masses are 4.352(225)GeV, 4.379(149)GeV and 7.315(257)GeV, completely "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0512044","kind":"arxiv","version":3},"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-lat/0512044","created_at":"2026-05-18T02:37:20.097833+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0512044v3","created_at":"2026-05-18T02:37:20.097833+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0512044","created_at":"2026-05-18T02:37:20.097833+00:00"},{"alias_kind":"pith_short_12","alias_value":"4LKR7QLNESJE","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_16","alias_value":"4LKR7QLNESJEEVXJ","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_8","alias_value":"4LKR7QLN","created_at":"2026-05-18T12:25:52.687210+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2503.00552","citing_title":"Study of $1^{--}$ P wave charmoniumlike and bottomoniumlike tetraquark spectroscopy","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H","json":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H.json","graph_json":"https://pith.science/api/pith-number/4LKR7QLNESJEEVXJFPKOPC6T2H/graph.json","events_json":"https://pith.science/api/pith-number/4LKR7QLNESJEEVXJFPKOPC6T2H/events.json","paper":"https://pith.science/paper/4LKR7QLN"},"agent_actions":{"view_html":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H","download_json":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H.json","view_paper":"https://pith.science/paper/4LKR7QLN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0512044&json=true","fetch_graph":"https://pith.science/api/pith-number/4LKR7QLNESJEEVXJFPKOPC6T2H/graph.json","fetch_events":"https://pith.science/api/pith-number/4LKR7QLNESJEEVXJFPKOPC6T2H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H/action/storage_attestation","attest_author":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H/action/author_attestation","sign_citation":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H/action/citation_signature","submit_replication":"https://pith.science/pith/4LKR7QLNESJEEVXJFPKOPC6T2H/action/replication_record"}},"created_at":"2026-05-18T02:37:20.097833+00:00","updated_at":"2026-05-18T02:37:20.097833+00:00"}