{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:EWKBXAVA6KXGTYDBXSRTCETE4X","short_pith_number":"pith:EWKBXAVA","schema_version":"1.0","canonical_sha256":"25941b82a0f2ae69e061bca3311264e5df0aa60a6fb06718e04b13020847e908","source":{"kind":"arxiv","id":"1410.6259","version":2},"attestation_state":"computed","paper":{"title":"Exploring the Spectrum of Heavy Quarkonium Hybrids with QCD Sum Rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Bulthuis, D. Harnett, J. Ho, R. T. Kleiv, Shi-Lin Zhu, T. G. Steele, T. Richards, Wei Chen","submitted_at":"2014-10-23T06:35:53Z","abstract_excerpt":"QCD Laplace sum rules are used to calculate heavy quarkonium (charmonium and bottomonium) hybrid masses in several distinct $J^{PC}$ channels. Previous studies of heavy quarkonium hybrids did not include the effects of dimension-six condensates, leading to unstable sum rules and unreliable mass predictions in some channels. We have updated these sum rules to include dimension-six condensates, providing new mass predictions for the spectra of heavy quarkonium hybrids. We confirm the finding of other approaches that the negative-parity $J^{PC}=(0,1,2)^{-+},\\,1^{--}$ states form the lightest hybr"},"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":"1410.6259","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-10-23T06:35:53Z","cross_cats_sorted":[],"title_canon_sha256":"54a51cd6104577aa2fa7af1dfebf706bbfaa4d7ed9a4efdd4cf6eb5f2991c900","abstract_canon_sha256":"a3b1cc391906aaad648d12e815dcecfc6363c78abe2f1c9b867ba1294b900c92"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:33.553805Z","signature_b64":"u5z4FOy5L3ppIFBJ8gPAla6CSzX63G98UHvFdWAmCosJZhjT+4oKw/LxbtsXWe/SGiqttDNa906q4FQlPZNTCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25941b82a0f2ae69e061bca3311264e5df0aa60a6fb06718e04b13020847e908","last_reissued_at":"2026-05-18T02:17:33.553143Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:33.553143Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring the Spectrum of Heavy Quarkonium Hybrids with QCD Sum Rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Bulthuis, D. Harnett, J. Ho, R. T. Kleiv, Shi-Lin Zhu, T. G. Steele, T. Richards, Wei Chen","submitted_at":"2014-10-23T06:35:53Z","abstract_excerpt":"QCD Laplace sum rules are used to calculate heavy quarkonium (charmonium and bottomonium) hybrid masses in several distinct $J^{PC}$ channels. Previous studies of heavy quarkonium hybrids did not include the effects of dimension-six condensates, leading to unstable sum rules and unreliable mass predictions in some channels. We have updated these sum rules to include dimension-six condensates, providing new mass predictions for the spectra of heavy quarkonium hybrids. We confirm the finding of other approaches that the negative-parity $J^{PC}=(0,1,2)^{-+},\\,1^{--}$ states form the lightest hybr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.6259","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":"1410.6259","created_at":"2026-05-18T02:17:33.553261+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.6259v2","created_at":"2026-05-18T02:17:33.553261+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.6259","created_at":"2026-05-18T02:17:33.553261+00:00"},{"alias_kind":"pith_short_12","alias_value":"EWKBXAVA6KXG","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_16","alias_value":"EWKBXAVA6KXGTYDB","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_8","alias_value":"EWKBXAVA","created_at":"2026-05-18T12:28:28.263976+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X","json":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X.json","graph_json":"https://pith.science/api/pith-number/EWKBXAVA6KXGTYDBXSRTCETE4X/graph.json","events_json":"https://pith.science/api/pith-number/EWKBXAVA6KXGTYDBXSRTCETE4X/events.json","paper":"https://pith.science/paper/EWKBXAVA"},"agent_actions":{"view_html":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X","download_json":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X.json","view_paper":"https://pith.science/paper/EWKBXAVA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.6259&json=true","fetch_graph":"https://pith.science/api/pith-number/EWKBXAVA6KXGTYDBXSRTCETE4X/graph.json","fetch_events":"https://pith.science/api/pith-number/EWKBXAVA6KXGTYDBXSRTCETE4X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X/action/storage_attestation","attest_author":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X/action/author_attestation","sign_citation":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X/action/citation_signature","submit_replication":"https://pith.science/pith/EWKBXAVA6KXGTYDBXSRTCETE4X/action/replication_record"}},"created_at":"2026-05-18T02:17:33.553261+00:00","updated_at":"2026-05-18T02:17:33.553261+00:00"}