{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:WDEVJGLL6PQMA6ZLBZFYXZ3MCE","short_pith_number":"pith:WDEVJGLL","schema_version":"1.0","canonical_sha256":"b0c954996bf3e0c07b2b0e4b8be76c111b1b31ca9701765f1a200d318b0693f5","source":{"kind":"arxiv","id":"2403.04878","version":2},"attestation_state":"computed","paper":{"title":"Reappraisal of SU(3)-flavor breaking in $B\\rightarrow DP$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Amarjit Soni, Jonathan Davies, Nicola Skidmore, Stefan Schacht","submitted_at":"2024-03-07T19:56:19Z","abstract_excerpt":"In light of recently found deviations of the experimental data from predictions from QCD factorization for $B_{(s)}\\rightarrow D_{(s)}P$ decays, where $P=\\{\\pi,K\\}$, we systematically probe the current status of the SU(3)$_F$ expansion from a fit to experimental branching ratio data without any further theory input. We find that the current data are in agreement with the power counting of the SU(3)$_F$ expansion. While the SU(3)$_F$ limit is excluded at $>5\\sigma$, amplitude-level SU(3)$_F$-breaking contributions of $\\sim 20\\%$ suffice for an excellent description of the data. SU(3)$_F$ breaki"},"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":"2403.04878","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-07T19:56:19Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"ef3c9ac590d2d273ee183125971dc075a2f1c11c659d93dd9526d34edaa4c64d","abstract_canon_sha256":"0295926e83522d91fa81ff76643777651e6433be44229d442da2ffe45602168a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:36:23.333675Z","signature_b64":"eLtCiw98c0eyY+6IL+EVDNmplmRghZyJEzdMdTRPVal7D0yPQJAzaFDOQDsFTb87mtFbD8Ss24hQpR2grY4MDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0c954996bf3e0c07b2b0e4b8be76c111b1b31ca9701765f1a200d318b0693f5","last_reissued_at":"2026-07-05T08:36:23.333151Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:36:23.333151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reappraisal of SU(3)-flavor breaking in $B\\rightarrow DP$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Amarjit Soni, Jonathan Davies, Nicola Skidmore, Stefan Schacht","submitted_at":"2024-03-07T19:56:19Z","abstract_excerpt":"In light of recently found deviations of the experimental data from predictions from QCD factorization for $B_{(s)}\\rightarrow D_{(s)}P$ decays, where $P=\\{\\pi,K\\}$, we systematically probe the current status of the SU(3)$_F$ expansion from a fit to experimental branching ratio data without any further theory input. We find that the current data are in agreement with the power counting of the SU(3)$_F$ expansion. While the SU(3)$_F$ limit is excluded at $>5\\sigma$, amplitude-level SU(3)$_F$-breaking contributions of $\\sim 20\\%$ suffice for an excellent description of the data. SU(3)$_F$ breaki"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.04878","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/2403.04878/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":"2403.04878","created_at":"2026-07-05T08:36:23.333227+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.04878v2","created_at":"2026-07-05T08:36:23.333227+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.04878","created_at":"2026-07-05T08:36:23.333227+00:00"},{"alias_kind":"pith_short_12","alias_value":"WDEVJGLL6PQM","created_at":"2026-07-05T08:36:23.333227+00:00"},{"alias_kind":"pith_short_16","alias_value":"WDEVJGLL6PQMA6ZL","created_at":"2026-07-05T08:36:23.333227+00:00"},{"alias_kind":"pith_short_8","alias_value":"WDEVJGLL","created_at":"2026-07-05T08:36:23.333227+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.25998","citing_title":"New insights into the $b\\rightarrow c \\bar{u}q$ puzzle through Top-Bottom synergies","ref_index":50,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE","json":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE.json","graph_json":"https://pith.science/api/pith-number/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/graph.json","events_json":"https://pith.science/api/pith-number/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/events.json","paper":"https://pith.science/paper/WDEVJGLL"},"agent_actions":{"view_html":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE","download_json":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE.json","view_paper":"https://pith.science/paper/WDEVJGLL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.04878&json=true","fetch_graph":"https://pith.science/api/pith-number/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/graph.json","fetch_events":"https://pith.science/api/pith-number/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/action/storage_attestation","attest_author":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/action/author_attestation","sign_citation":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/action/citation_signature","submit_replication":"https://pith.science/pith/WDEVJGLL6PQMA6ZLBZFYXZ3MCE/action/replication_record"}},"created_at":"2026-07-05T08:36:23.333227+00:00","updated_at":"2026-07-05T08:36:23.333227+00:00"}