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In doing operator production expansion at QCD side, the contributions of the perturbative part, vacuum condensate terms of $\\langle{\\bar qq}\\rangle$, $\\langle g_{s}^{2}GG\\rangle$, $\\langle \\bar q g_{s}\\sigma Gq\\rangle$ and $g_{s}^{2}\\langle{\\b","authors_text":"Bin Wu, Guo-Liang Yu, Jie Lu, Peng Yang, Ze Zhou, Zhi-Gang Wang","cross_cats":[],"headline":"QCD sum rules calculate form factors for 1/2+ to 3/2+ weak transitions in doubly charmed baryons and predict rates for their semileptonic decays.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-01-10T05:02:54Z","title":"Analysis of the semileptonic decays of $\\Xi_{cc}$ and $\\Omega_{cc}$ baryons in QCD sum rules"},"references":{"count":82,"internal_anchors":1,"resolved_work":82,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"u(p, s) and uα(p′, s′) denote the spinor wave functions of initial ( B1) and final ( B∗","work_id":"3a6e76b9-cce5-49d3-b211-109c9806c0ae","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Fi(q2) and Gi(q2) (i = 1 ∼4) are the vector and axial vector form factors with q = p −p′","work_id":"70a0d024-2501-4834-8b19-0545f98e8229","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"In the phenomenological side, a complete sets of hadron states which can couple to the corresponding interpolating currents are inserted into the correlation function","work_id":"a0114298-104f-42c7-b857-06456c135bfb","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"and (10) for ΠQCD−V µν and ΠQCD−A µν , respectively. 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These scalar invariant amplitudes can be repres","work_id":"1967f2dd-732e-4dda-980a-5f12f82959d8","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"The superscript 0 denotes that the dimension of perturbativ e term is zero","work_id":"a5f4022a-a3a2-4125-91c6-de89a28a6065","year":null}],"snapshot_sha256":"d4abaea0a5b63458f668033767964fcd022ce73d8c77d7428767682c3dd20e9a"},"source":{"id":"2601.06427","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-16T16:05:03.548030Z","id":"4b685bf4-b655-4289-994b-223b573cb890","model_set":{"reader":"grok-4.3"},"one_line_summary":"QCD sum rules yield form factors that are extrapolated to predict semileptonic decay widths for Ξ_cc^{++} and Ω_cc^+ baryons into singly charmed states plus lepton-neutrino pairs.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"QCD sum rules calculate form factors for 1/2+ to 3/2+ weak transitions in doubly charmed baryons and predict rates for their semileptonic decays.","strongest_claim":"Using the predicted form factors, we finally analyze the semileptonic decays of Ξ_cc^{++}→Σ_c^{*+}l^+ν_l, Ξ_cc^{++}→Ξ_c^{′*+}l^+ν_l, Ω_cc^+→Ξ_c^{′*0}l^+ν_l and Ω_cc^+→Ω_c^{*0}l^+ν_l with l=e,μ.","weakest_assumption":"The numerical results obtained in the space-like region are extrapolated into the time-like region by a fitting function whose functional form is chosen without independent justification from first principles."}},"verdict_id":"4b685bf4-b655-4289-994b-223b573cb890"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:6f24b425c8da38e5bdb08def4a238e43c04bb45af7734d9fe6e0278632afeea1","target":"record","created_at":"2026-06-11T01:09:26Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"f7291f5f604f656505bc330213b58d9796e1f4eac0658fc9e970d21f81543de5","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-01-10T05:02:54Z","title_canon_sha256":"f7cac9d9db2821298cc45147e5289150f1e71ee865fa565a168e7af4816046ec"},"schema_version":"1.0","source":{"id":"2601.06427","kind":"arxiv","version":2}},"canonical_sha256":"56bc4f28ffb7a08db022f6a1ca6e587da055859c30d46d59fbf9508c52597e0a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"56bc4f28ffb7a08db022f6a1ca6e587da055859c30d46d59fbf9508c52597e0a","first_computed_at":"2026-06-11T01:09:26.415298Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-11T01:09:26.415298Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ND+S3OGobLcgIfdl+84aUXfHg4cYKTk5YUcf6Qy5SSkA9xhr7dDRq9Wta/x6ZTg/YY2+3qD6iOs50YRaGNViDA==","signature_status":"signed_v1","signed_at":"2026-06-11T01:09:26.416383Z","signed_message":"canonical_sha256_bytes"},"source_id":"2601.06427","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6f24b425c8da38e5bdb08def4a238e43c04bb45af7734d9fe6e0278632afeea1","sha256:9218b8ae656b17d59007cfb3d4d6fade80ef430c18b7d2f88d109ca94bf70c4e"],"state_sha256":"830b23296905caf4e82599fc7e064e040474d8d5f5eaf84488e544ebf19a4742"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I6przelC6Icv3M+BJXZjfxxUfAqsOwpS5j1F4roSWC/6UXZISG+0NIV5tO4bazy7KheleAJi66yIZvzkR+bnBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T17:52:10.623621Z","bundle_sha256":"d80107b8059ec113ed8e9d6ef6b11e314d7559cbb861f02be0e6485f926194b1"}}