{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:EKINMYODK2VVRM2APUZCHZLP7L","short_pith_number":"pith:EKINMYOD","schema_version":"1.0","canonical_sha256":"2290d661c356ab58b3407d3223e56ffad11b8e2ba6e613957e99bff4bc43ad9c","source":{"kind":"arxiv","id":"2307.05090","version":4},"attestation_state":"computed","paper":{"title":"The strong vertices of bottom mesons $B$, $B^{*}$ and bottomonia $\\Upsilon$, $\\eta_{b}$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bin Wu, Guo-Liang Yu, Jie Lu, Zhi-Gang Wang","submitted_at":"2023-07-11T07:43:38Z","abstract_excerpt":"In this article, the strong coupling constants of vertices $BB\\Upsilon$, $BB^{*}\\Upsilon$, $B^{*}B^{*}\\Upsilon$, $BB^{*}\\eta_{b}$ and $B^{*}B^{*}\\eta_{b}$ are analyzed in the framework of QCD sum rules. In this work, all possible off-shell cases and the contributions of vacuum condensate terms including $\\langle\\overline{q}q\\rangle$, $\\langle\\overline{q}g_{s}\\sigma Gq\\rangle$, $\\langle g_{s}^{2}G^{2}\\rangle$, $\\langle f^{3}G^{3}\\rangle$ and $\\langle\\overline{q}q\\rangle\\langle g_{s}^{2}G^{2}\\rangle$ are considered. The momentum dependent strong coupling constants are first calculated and then a"},"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":"2307.05090","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-11T07:43:38Z","cross_cats_sorted":[],"title_canon_sha256":"a549d77e39e564de3d797620a656419adbcb8b499be60640bfddb0ec12fe6191","abstract_canon_sha256":"a96c8582b789353ecc10acd506a60416d0e35a7843b4bd877528a60c15a48bf9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:37:50.296121Z","signature_b64":"KzlA2QkQ/hTFw6wJO6qu+PkC4u0l9RZphURBiUREsNglgiz94tlrkQ0QAUhJR8fcWcvDLCqTipvrB7BmAwWzBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2290d661c356ab58b3407d3223e56ffad11b8e2ba6e613957e99bff4bc43ad9c","last_reissued_at":"2026-07-05T07:37:50.295696Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:37:50.295696Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The strong vertices of bottom mesons $B$, $B^{*}$ and bottomonia $\\Upsilon$, $\\eta_{b}$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bin Wu, Guo-Liang Yu, Jie Lu, Zhi-Gang Wang","submitted_at":"2023-07-11T07:43:38Z","abstract_excerpt":"In this article, the strong coupling constants of vertices $BB\\Upsilon$, $BB^{*}\\Upsilon$, $B^{*}B^{*}\\Upsilon$, $BB^{*}\\eta_{b}$ and $B^{*}B^{*}\\eta_{b}$ are analyzed in the framework of QCD sum rules. In this work, all possible off-shell cases and the contributions of vacuum condensate terms including $\\langle\\overline{q}q\\rangle$, $\\langle\\overline{q}g_{s}\\sigma Gq\\rangle$, $\\langle g_{s}^{2}G^{2}\\rangle$, $\\langle f^{3}G^{3}\\rangle$ and $\\langle\\overline{q}q\\rangle\\langle g_{s}^{2}G^{2}\\rangle$ are considered. The momentum dependent strong coupling constants are first calculated and then a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.05090","kind":"arxiv","version":4},"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/2307.05090/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":"2307.05090","created_at":"2026-07-05T07:37:50.295754+00:00"},{"alias_kind":"arxiv_version","alias_value":"2307.05090v4","created_at":"2026-07-05T07:37:50.295754+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.05090","created_at":"2026-07-05T07:37:50.295754+00:00"},{"alias_kind":"pith_short_12","alias_value":"EKINMYODK2VV","created_at":"2026-07-05T07:37:50.295754+00:00"},{"alias_kind":"pith_short_16","alias_value":"EKINMYODK2VVRM2A","created_at":"2026-07-05T07:37:50.295754+00:00"},{"alias_kind":"pith_short_8","alias_value":"EKINMYOD","created_at":"2026-07-05T07:37:50.295754+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.11900","citing_title":"Analysis of the semileptonic decays $\\Lambda_b\\to\\Lambda_cl\\bar{\\nu}_l$ and $\\Xi_b\\to\\Xi_cl\\bar{\\nu}_l$ in QCD sum rules","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L","json":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L.json","graph_json":"https://pith.science/api/pith-number/EKINMYODK2VVRM2APUZCHZLP7L/graph.json","events_json":"https://pith.science/api/pith-number/EKINMYODK2VVRM2APUZCHZLP7L/events.json","paper":"https://pith.science/paper/EKINMYOD"},"agent_actions":{"view_html":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L","download_json":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L.json","view_paper":"https://pith.science/paper/EKINMYOD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2307.05090&json=true","fetch_graph":"https://pith.science/api/pith-number/EKINMYODK2VVRM2APUZCHZLP7L/graph.json","fetch_events":"https://pith.science/api/pith-number/EKINMYODK2VVRM2APUZCHZLP7L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L/action/storage_attestation","attest_author":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L/action/author_attestation","sign_citation":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L/action/citation_signature","submit_replication":"https://pith.science/pith/EKINMYODK2VVRM2APUZCHZLP7L/action/replication_record"}},"created_at":"2026-07-05T07:37:50.295754+00:00","updated_at":"2026-07-05T07:37:50.295754+00:00"}