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The contributions of two gluon condensates as a radiative correction are considered. The results show that g$_{h_{b}B_{c}^{PS}B_{c}^{V}}=8.80\\pm 2.84 GeV^{-1}$and g$_{h_{b}B_{c}^{V} B_{c}^{PS}}=9.34\\pm 3.12 GeV^{-1}$ in the $B_{c}^{PS}$ and $B_{c}^{V}$ off-shell state, respectively."},"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":"1401.4090","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-16T16:59:34Z","cross_cats_sorted":[],"title_canon_sha256":"c0d368a22185b974571f053b17a69dc1246e992b2c9b35f302729324bc9b989d","abstract_canon_sha256":"65573ee34327c1427a2a8ce972edb20d3af96def7ee5fde2d53772221bdb0656"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:24.784612Z","signature_b64":"9OKJEUp/Qxuns0pjqNrM1irEBUwnUagCQruriqfQwzryD7zkZa2kRcBxWYr5UAui93qfeuCN6rMdVmEpKs22AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"19947f59a0d71e1750d6c15096d3ae94e5149cd3bd388e2cc8955baa29696a06","last_reissued_at":"2026-05-18T01:45:24.784189Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:24.784189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong coupling constant of h$_{b}$ vector to the pseudoscalar and vector $B_{c}$ mesons in QCD sum rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Abbasi, V. Bashiry","submitted_at":"2014-01-16T16:59:34Z","abstract_excerpt":"The strong coupling constant g$_{h_{b}B_{c}^{PS}B_{c}^{V}}$ is calculated using the three-point QCD sum rules method. We use correlation functions to obtain these strong coupling constants with contributions of both B$_{c}^{PS} $ and B$_{c}^{V}$mesons as off-shell states. The contributions of two gluon condensates as a radiative correction are considered. The results show that g$_{h_{b}B_{c}^{PS}B_{c}^{V}}=8.80\\pm 2.84 GeV^{-1}$and g$_{h_{b}B_{c}^{V} B_{c}^{PS}}=9.34\\pm 3.12 GeV^{-1}$ in the $B_{c}^{PS}$ and $B_{c}^{V}$ off-shell state, respectively."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.4090","kind":"arxiv","version":1},"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":"1401.4090","created_at":"2026-05-18T01:45:24.784261+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.4090v1","created_at":"2026-05-18T01:45:24.784261+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.4090","created_at":"2026-05-18T01:45:24.784261+00:00"},{"alias_kind":"pith_short_12","alias_value":"DGKH6WNA24PB","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_16","alias_value":"DGKH6WNA24PBOUGW","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_8","alias_value":"DGKH6WNA","created_at":"2026-05-18T12:28:25.294606+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/DGKH6WNA24PBOUGWYFIJNU5OST","json":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST.json","graph_json":"https://pith.science/api/pith-number/DGKH6WNA24PBOUGWYFIJNU5OST/graph.json","events_json":"https://pith.science/api/pith-number/DGKH6WNA24PBOUGWYFIJNU5OST/events.json","paper":"https://pith.science/paper/DGKH6WNA"},"agent_actions":{"view_html":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST","download_json":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST.json","view_paper":"https://pith.science/paper/DGKH6WNA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.4090&json=true","fetch_graph":"https://pith.science/api/pith-number/DGKH6WNA24PBOUGWYFIJNU5OST/graph.json","fetch_events":"https://pith.science/api/pith-number/DGKH6WNA24PBOUGWYFIJNU5OST/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST/action/storage_attestation","attest_author":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST/action/author_attestation","sign_citation":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST/action/citation_signature","submit_replication":"https://pith.science/pith/DGKH6WNA24PBOUGWYFIJNU5OST/action/replication_record"}},"created_at":"2026-05-18T01:45:24.784261+00:00","updated_at":"2026-05-18T01:45:24.784261+00:00"}