{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:LWDN3XNE5X2ERWPEY44TBQYUTZ","short_pith_number":"pith:LWDN3XNE","schema_version":"1.0","canonical_sha256":"5d86dddda4edf448d9e4c73930c3149e5c1c60b1d6f68f5d7747dd1445101a4f","source":{"kind":"arxiv","id":"1112.3896","version":2},"attestation_state":"computed","paper":{"title":"B0 meson decays to rho0 K*0, f0 K*0, and rho-K*+, including higher K* resonances","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The BABAR Collaboration","submitted_at":"2011-12-16T17:27:26Z","abstract_excerpt":"We present branching fraction measurements for the decays B0 -> rho0 K*0, B0 -> f0 K*0, and B0 -> rho- K*+, where K* is an S-wave (K pi)_0* or a K*(892) meson; we also measure B0 -> f0 K_2*(1430)^0. For the K*(892) channels, we report measurements of longitudinal polarization fractions (for rho final states) and direct CP-violation asymmetries. These results are obtained from a sample of (471.0 +/- 2.8) x 10^6 BBbar pairs collected with the BaBar detector at the PEP-II asymmetric-energy e+ e- collider at the SLAC National Accelerator Laboratory. We observe rho0 K*(892)^0, rho0 (K pi)_0^{*0}, f"},"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":"1112.3896","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-12-16T17:27:26Z","cross_cats_sorted":[],"title_canon_sha256":"389c9ecefbf67e29b0dd77eb8729527b0e29031b014ef5e475805ee8ad4ec9d1","abstract_canon_sha256":"be13f3783fb039b1e4777d17005a8c7f87777cd0bb4aa7f61d69966db1521dd8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:53.961535Z","signature_b64":"AtOfY/Gft5ZblWCA7WRXc5PkFNLvCVXFbVEG64ltAhfHXPdadK+pxzjJf5Wd6SQ5owRj7tOoeLN0/c5nayY3DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d86dddda4edf448d9e4c73930c3149e5c1c60b1d6f68f5d7747dd1445101a4f","last_reissued_at":"2026-05-18T03:22:53.960960Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:53.960960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"B0 meson decays to rho0 K*0, f0 K*0, and rho-K*+, including higher K* resonances","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The BABAR Collaboration","submitted_at":"2011-12-16T17:27:26Z","abstract_excerpt":"We present branching fraction measurements for the decays B0 -> rho0 K*0, B0 -> f0 K*0, and B0 -> rho- K*+, where K* is an S-wave (K pi)_0* or a K*(892) meson; we also measure B0 -> f0 K_2*(1430)^0. For the K*(892) channels, we report measurements of longitudinal polarization fractions (for rho final states) and direct CP-violation asymmetries. These results are obtained from a sample of (471.0 +/- 2.8) x 10^6 BBbar pairs collected with the BaBar detector at the PEP-II asymmetric-energy e+ e- collider at the SLAC National Accelerator Laboratory. We observe rho0 K*(892)^0, rho0 (K pi)_0^{*0}, f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3896","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":"1112.3896","created_at":"2026-05-18T03:22:53.961038+00:00"},{"alias_kind":"arxiv_version","alias_value":"1112.3896v2","created_at":"2026-05-18T03:22:53.961038+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3896","created_at":"2026-05-18T03:22:53.961038+00:00"},{"alias_kind":"pith_short_12","alias_value":"LWDN3XNE5X2E","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_16","alias_value":"LWDN3XNE5X2ERWPE","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_8","alias_value":"LWDN3XNE","created_at":"2026-05-18T12:26:34.985390+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.13563","citing_title":"First observation of $CP$ violation and measurement of polarization in $B^+\\to\\rho(770)^0 K^*(892)^+$ decays","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ","json":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ.json","graph_json":"https://pith.science/api/pith-number/LWDN3XNE5X2ERWPEY44TBQYUTZ/graph.json","events_json":"https://pith.science/api/pith-number/LWDN3XNE5X2ERWPEY44TBQYUTZ/events.json","paper":"https://pith.science/paper/LWDN3XNE"},"agent_actions":{"view_html":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ","download_json":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ.json","view_paper":"https://pith.science/paper/LWDN3XNE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1112.3896&json=true","fetch_graph":"https://pith.science/api/pith-number/LWDN3XNE5X2ERWPEY44TBQYUTZ/graph.json","fetch_events":"https://pith.science/api/pith-number/LWDN3XNE5X2ERWPEY44TBQYUTZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ/action/storage_attestation","attest_author":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ/action/author_attestation","sign_citation":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ/action/citation_signature","submit_replication":"https://pith.science/pith/LWDN3XNE5X2ERWPEY44TBQYUTZ/action/replication_record"}},"created_at":"2026-05-18T03:22:53.961038+00:00","updated_at":"2026-05-18T03:22:53.961038+00:00"}