{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:EBIPI52PP4R3WHVJQAVCQT4XVF","short_pith_number":"pith:EBIPI52P","schema_version":"1.0","canonical_sha256":"2050f4774f7f23bb1ea9802a284f97a95863363115b78d0d412d447f90f6163a","source":{"kind":"arxiv","id":"2407.07431","version":2},"attestation_state":"computed","paper":{"title":"Light-cone sum rules study on the purely non-factorizable $\\Lambda_{c}^{+}\\to\\Xi^{0}K^{+}$ decay","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Yu-Ji Shi, Zhen-Xing Zhao","submitted_at":"2024-07-10T07:35:11Z","abstract_excerpt":"We investigate the purely non-factorizable $\\Lambda_{c}^{+}\\to\\Xi^{0}K^{+}$ decay using light-cone sum rules. To extract the decay amplitudes, a three-point correlation function is defined and calculated at hadron and quark-gluon level, respectively. Both the W-exchange and the W-inward emission diagrams are considered in the quark-gluon level calculation, where the two-particle light-cone distribution amplitudes (LCDAs) of kaon are used as non-perturbative input. We obtain the decay amplitudes contributed from the twist-2 and twist-3 kaon LCDAs, respectively. The obtained P-wave amplitude is "},"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":"2407.07431","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-07-10T07:35:11Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"cadb6e24be3becd8e45378264120c7cd49da2df12a5a009ce36712acea767a3a","abstract_canon_sha256":"930a16ea10926f2ec4a5321713773cbd87ca758901e7c5aa937c79d294cb8af6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:43:57.325817Z","signature_b64":"5kteYLcPtTyibFPM1D5uILRe7pAp2g+OY2ADLZOmSGV2hrMdpPvokkBGjnWq8HapjpObiQaHVfSddwRIvUVTDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2050f4774f7f23bb1ea9802a284f97a95863363115b78d0d412d447f90f6163a","last_reissued_at":"2026-07-05T08:43:57.325386Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:43:57.325386Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light-cone sum rules study on the purely non-factorizable $\\Lambda_{c}^{+}\\to\\Xi^{0}K^{+}$ decay","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Yu-Ji Shi, Zhen-Xing Zhao","submitted_at":"2024-07-10T07:35:11Z","abstract_excerpt":"We investigate the purely non-factorizable $\\Lambda_{c}^{+}\\to\\Xi^{0}K^{+}$ decay using light-cone sum rules. To extract the decay amplitudes, a three-point correlation function is defined and calculated at hadron and quark-gluon level, respectively. Both the W-exchange and the W-inward emission diagrams are considered in the quark-gluon level calculation, where the two-particle light-cone distribution amplitudes (LCDAs) of kaon are used as non-perturbative input. We obtain the decay amplitudes contributed from the twist-2 and twist-3 kaon LCDAs, respectively. The obtained P-wave amplitude is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.07431","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2407.07431/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":"2407.07431","created_at":"2026-07-05T08:43:57.325443+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.07431v2","created_at":"2026-07-05T08:43:57.325443+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.07431","created_at":"2026-07-05T08:43:57.325443+00:00"},{"alias_kind":"pith_short_12","alias_value":"EBIPI52PP4R3","created_at":"2026-07-05T08:43:57.325443+00:00"},{"alias_kind":"pith_short_16","alias_value":"EBIPI52PP4R3WHVJ","created_at":"2026-07-05T08:43:57.325443+00:00"},{"alias_kind":"pith_short_8","alias_value":"EBIPI52P","created_at":"2026-07-05T08:43:57.325443+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.04311","citing_title":"Analysis of the semileptonic decays $\\Sigma_b\\to\\Sigma_cl\\bar{\\nu}_l$, $\\Xi'_b\\to\\Xi'_cl\\bar{\\nu}_l$ and $\\Omega_b\\to\\Omega_cl\\bar{\\nu}_l$ in QCD sum rules","ref_index":16,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF","json":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF.json","graph_json":"https://pith.science/api/pith-number/EBIPI52PP4R3WHVJQAVCQT4XVF/graph.json","events_json":"https://pith.science/api/pith-number/EBIPI52PP4R3WHVJQAVCQT4XVF/events.json","paper":"https://pith.science/paper/EBIPI52P"},"agent_actions":{"view_html":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF","download_json":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF.json","view_paper":"https://pith.science/paper/EBIPI52P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.07431&json=true","fetch_graph":"https://pith.science/api/pith-number/EBIPI52PP4R3WHVJQAVCQT4XVF/graph.json","fetch_events":"https://pith.science/api/pith-number/EBIPI52PP4R3WHVJQAVCQT4XVF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF/action/storage_attestation","attest_author":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF/action/author_attestation","sign_citation":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF/action/citation_signature","submit_replication":"https://pith.science/pith/EBIPI52PP4R3WHVJQAVCQT4XVF/action/replication_record"}},"created_at":"2026-07-05T08:43:57.325443+00:00","updated_at":"2026-07-05T08:43:57.325443+00:00"}