{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:3F74PGHAW3AMJYFYNJL23WDAKR","short_pith_number":"pith:3F74PGHA","schema_version":"1.0","canonical_sha256":"d97fc798e0b6c0c4e0b86a57add8605467ebf3f7cda5f2578d6ba656217fe2b0","source":{"kind":"arxiv","id":"2607.16697","version":1},"attestation_state":"computed","paper":{"title":"The semileptonic decays of $\\mathcal{B}_{Q_{1}Q_{2}}(\\frac{1}{2}^{+})\\rightarrow\\mathcal{B}_{Q_{1}}^{*}(\\frac{3}{2}^{+})$ in QCD sum rules","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bin Wu, Guo-Liang Yu, Jie Lu, Peng Yang, Ze Zhou, Zhi-Gang Wang","submitted_at":"2026-07-18T08:12:59Z","abstract_excerpt":"In the framework of QCD sum rules, we systematically analyze the weak transition process $\\mathcal{B}_{Q_{1}Q_{2}}(\\frac{1}{2}^{+})\\rightarrow\\mathcal{B}_{Q_{1}}^{*}(\\frac{3}{2}^{+})$. When doing the operator product expansion in the QCD side, we consider the contributions of perturbative part and vacuum condensate terms up to dimension 6. In the phenomenological side, we eliminate the interferences of the low spin states and negative parity states by employing 16 different dirac structures. As an application, these form factors are finally used to analyze the semileptonic decays of $\\mathcal{"},"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":"2607.16697","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-18T08:12:59Z","cross_cats_sorted":[],"title_canon_sha256":"19896ff21b17709717945bd841d4d9068b48f94bc4aee216426f67a43c001216","abstract_canon_sha256":"ddc02d244517e4a5e71852d8e14368b0446ca1ac9e73aef1c4713cbd1d42ac73"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-21T01:20:22.478698Z","signature_b64":"l7sYTrmrK9vWowGT4sAMV+HZpVDNbpIwyKCzn+OzleaIYkHwANXlE+5M+W/A3IoStUl9bPTSex0rKdJiXNXGAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d97fc798e0b6c0c4e0b86a57add8605467ebf3f7cda5f2578d6ba656217fe2b0","last_reissued_at":"2026-07-21T01:20:22.477865Z","signature_status":"signed_v1","first_computed_at":"2026-07-21T01:20:22.477865Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The semileptonic decays of $\\mathcal{B}_{Q_{1}Q_{2}}(\\frac{1}{2}^{+})\\rightarrow\\mathcal{B}_{Q_{1}}^{*}(\\frac{3}{2}^{+})$ in QCD sum rules","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bin Wu, Guo-Liang Yu, Jie Lu, Peng Yang, Ze Zhou, Zhi-Gang Wang","submitted_at":"2026-07-18T08:12:59Z","abstract_excerpt":"In the framework of QCD sum rules, we systematically analyze the weak transition process $\\mathcal{B}_{Q_{1}Q_{2}}(\\frac{1}{2}^{+})\\rightarrow\\mathcal{B}_{Q_{1}}^{*}(\\frac{3}{2}^{+})$. When doing the operator product expansion in the QCD side, we consider the contributions of perturbative part and vacuum condensate terms up to dimension 6. In the phenomenological side, we eliminate the interferences of the low spin states and negative parity states by employing 16 different dirac structures. As an application, these form factors are finally used to analyze the semileptonic decays of $\\mathcal{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.16697","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.16697/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":"2607.16697","created_at":"2026-07-21T01:20:22.478277+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.16697v1","created_at":"2026-07-21T01:20:22.478277+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.16697","created_at":"2026-07-21T01:20:22.478277+00:00"},{"alias_kind":"pith_short_12","alias_value":"3F74PGHAW3AM","created_at":"2026-07-21T01:20:22.478277+00:00"},{"alias_kind":"pith_short_16","alias_value":"3F74PGHAW3AMJYFY","created_at":"2026-07-21T01:20:22.478277+00:00"},{"alias_kind":"pith_short_8","alias_value":"3F74PGHA","created_at":"2026-07-21T01:20:22.478277+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/3F74PGHAW3AMJYFYNJL23WDAKR","json":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR.json","graph_json":"https://pith.science/api/pith-number/3F74PGHAW3AMJYFYNJL23WDAKR/graph.json","events_json":"https://pith.science/api/pith-number/3F74PGHAW3AMJYFYNJL23WDAKR/events.json","paper":"https://pith.science/paper/3F74PGHA"},"agent_actions":{"view_html":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR","download_json":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR.json","view_paper":"https://pith.science/paper/3F74PGHA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.16697&json=true","fetch_graph":"https://pith.science/api/pith-number/3F74PGHAW3AMJYFYNJL23WDAKR/graph.json","fetch_events":"https://pith.science/api/pith-number/3F74PGHAW3AMJYFYNJL23WDAKR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR/action/storage_attestation","attest_author":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR/action/author_attestation","sign_citation":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR/action/citation_signature","submit_replication":"https://pith.science/pith/3F74PGHAW3AMJYFYNJL23WDAKR/action/replication_record"}},"created_at":"2026-07-21T01:20:22.478277+00:00","updated_at":"2026-07-21T01:20:22.478277+00:00"}