{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:ODCXERX3SX5NT5N25HLK2BVW2S","short_pith_number":"pith:ODCXERX3","schema_version":"1.0","canonical_sha256":"70c57246fb95fad9f5bae9d6ad06b6d4b94f095786ae2a9bcd7a9175c01f33b4","source":{"kind":"arxiv","id":"0904.1955","version":2},"attestation_state":"computed","paper":{"title":"B \\to K_0^*(1430) \\eta^{(\\prime)} decays in the pQCD approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Xin Liu, Zhen-jun Xiao, Zhi-Qing Zhang","submitted_at":"2009-04-13T15:00:17Z","abstract_excerpt":"Based on the assumption of two-quark structure of the scalar meson $K_0^*(1430)$, we calculate the CP-averaged branching ratios for $B \\to K_0^*(1430) \\etap$ decays in the framework of the perturbative QCD (pQCD) approach here. We perform the evaluations in two scenarios for the scalar meson spectrum. We find that: (a) the pQCD predictions for $Br(B \\to K_0^*(1430) \\eta^{(\\prime)})$ is $10^{-5} - 10^{-6}$, basically agree with the data within large theoretical uncertainty; (b) the agreement between the pQCD predictions and the data in the scenario I is better than that in the scenario II, whic"},"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":"0904.1955","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-04-13T15:00:17Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"96d77ef9d47eeadbbb8c847ee3a41329d20e862c3e3e8a0046d8a8da4a21ca57","abstract_canon_sha256":"4e1b4dfcd5c15be1a89b3ee54e5c3b9fd472f368c48d09a37c3a41db78f4afff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:02.029523Z","signature_b64":"boIGXYgavkoUtvi7y2Or6b7bpE8L3+j4Zxxf+DVmJCNHtOZt+s6baBMJUnLWuY57r6Hd1E6HpWJ6pqXw2fWoBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"70c57246fb95fad9f5bae9d6ad06b6d4b94f095786ae2a9bcd7a9175c01f33b4","last_reissued_at":"2026-05-18T04:25:02.029000Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:02.029000Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"B \\to K_0^*(1430) \\eta^{(\\prime)} decays in the pQCD approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Xin Liu, Zhen-jun Xiao, Zhi-Qing Zhang","submitted_at":"2009-04-13T15:00:17Z","abstract_excerpt":"Based on the assumption of two-quark structure of the scalar meson $K_0^*(1430)$, we calculate the CP-averaged branching ratios for $B \\to K_0^*(1430) \\etap$ decays in the framework of the perturbative QCD (pQCD) approach here. We perform the evaluations in two scenarios for the scalar meson spectrum. We find that: (a) the pQCD predictions for $Br(B \\to K_0^*(1430) \\eta^{(\\prime)})$ is $10^{-5} - 10^{-6}$, basically agree with the data within large theoretical uncertainty; (b) the agreement between the pQCD predictions and the data in the scenario I is better than that in the scenario II, whic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.1955","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":""},"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":"0904.1955","created_at":"2026-05-18T04:25:02.029069+00:00"},{"alias_kind":"arxiv_version","alias_value":"0904.1955v2","created_at":"2026-05-18T04:25:02.029069+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.1955","created_at":"2026-05-18T04:25:02.029069+00:00"},{"alias_kind":"pith_short_12","alias_value":"ODCXERX3SX5N","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"ODCXERX3SX5NT5N2","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"ODCXERX3","created_at":"2026-05-18T12:26:01.383474+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.04191","citing_title":"Systematic Analysis of $B_s \\to SP$ Decays in Perturbative QCD Approach","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S","json":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S.json","graph_json":"https://pith.science/api/pith-number/ODCXERX3SX5NT5N25HLK2BVW2S/graph.json","events_json":"https://pith.science/api/pith-number/ODCXERX3SX5NT5N25HLK2BVW2S/events.json","paper":"https://pith.science/paper/ODCXERX3"},"agent_actions":{"view_html":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S","download_json":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S.json","view_paper":"https://pith.science/paper/ODCXERX3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0904.1955&json=true","fetch_graph":"https://pith.science/api/pith-number/ODCXERX3SX5NT5N25HLK2BVW2S/graph.json","fetch_events":"https://pith.science/api/pith-number/ODCXERX3SX5NT5N25HLK2BVW2S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S/action/storage_attestation","attest_author":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S/action/author_attestation","sign_citation":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S/action/citation_signature","submit_replication":"https://pith.science/pith/ODCXERX3SX5NT5N25HLK2BVW2S/action/replication_record"}},"created_at":"2026-05-18T04:25:02.029069+00:00","updated_at":"2026-05-18T04:25:02.029069+00:00"}