{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:RY6OVYV5XNMPYXR7O2UOXIUWK7","short_pith_number":"pith:RY6OVYV5","schema_version":"1.0","canonical_sha256":"8e3ceae2bdbb58fc5e3f76a8eba29657eb8a6aa4d9c1e241225650459c2017cf","source":{"kind":"arxiv","id":"0905.3615","version":1},"attestation_state":"computed","paper":{"title":"Time-dependent amplitude analysis of B0 --> K0S pi+ pi-","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, the BABAR Collaboration: B. Aubert","submitted_at":"2009-05-22T07:29:27Z","abstract_excerpt":"We perform a time-dependent amplitude analysis of $B^0 \\to K^0_S\\pi^+\\pi^-$ decays to extract the CP violation parameters of $f_0(980) K^0_S$ and $\\rho^0(770) K^0_S$ and the direct CP asymmetry of $K^{*+}(892) \\pi^-$. The results are obtained from a data sample of $(383 \\pm 3) \\times 10^6$ $B\\bar{B}$ decays, collected with the BABAR detector at the PEP-II asymmetric-energy $B$ factory at SLAC. We find two solutions, with an equivalent goodness-of-fit. Including systematic and Dalitz plot model uncertainties, the combined confidence interval for values of the CP parameter $\\beta_{eff}$ in $B^0$"},"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":"0905.3615","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2009-05-22T07:29:27Z","cross_cats_sorted":[],"title_canon_sha256":"5e8ab45ae12235dd8c2fc3f31a288764b35244bcfcc9a5a0c4f047879eef28c5","abstract_canon_sha256":"f8db4c6603bce3f9cdf470413ceafabea9e8eeab799a95d513585627ddbb048e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:26:08.504710Z","signature_b64":"/YEE0fr176dxv3OK0fwflu/bGPlAHqBmhnZabBKpzswDh/VwyMgK9P6yMd+MoXAVwMZKysRJ8yT/481jJb6HAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e3ceae2bdbb58fc5e3f76a8eba29657eb8a6aa4d9c1e241225650459c2017cf","last_reissued_at":"2026-07-04T17:26:08.504291Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:26:08.504291Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Time-dependent amplitude analysis of B0 --> K0S pi+ pi-","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, the BABAR Collaboration: B. Aubert","submitted_at":"2009-05-22T07:29:27Z","abstract_excerpt":"We perform a time-dependent amplitude analysis of $B^0 \\to K^0_S\\pi^+\\pi^-$ decays to extract the CP violation parameters of $f_0(980) K^0_S$ and $\\rho^0(770) K^0_S$ and the direct CP asymmetry of $K^{*+}(892) \\pi^-$. The results are obtained from a data sample of $(383 \\pm 3) \\times 10^6$ $B\\bar{B}$ decays, collected with the BABAR detector at the PEP-II asymmetric-energy $B$ factory at SLAC. We find two solutions, with an equivalent goodness-of-fit. Including systematic and Dalitz plot model uncertainties, the combined confidence interval for values of the CP parameter $\\beta_{eff}$ in $B^0$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0905.3615","kind":"arxiv","version":1},"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/0905.3615/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":"0905.3615","created_at":"2026-07-04T17:26:08.504360+00:00"},{"alias_kind":"arxiv_version","alias_value":"0905.3615v1","created_at":"2026-07-04T17:26:08.504360+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0905.3615","created_at":"2026-07-04T17:26:08.504360+00:00"},{"alias_kind":"pith_short_12","alias_value":"RY6OVYV5XNMP","created_at":"2026-07-04T17:26:08.504360+00:00"},{"alias_kind":"pith_short_16","alias_value":"RY6OVYV5XNMPYXR7","created_at":"2026-07-04T17:26:08.504360+00:00"},{"alias_kind":"pith_short_8","alias_value":"RY6OVYV5","created_at":"2026-07-04T17:26:08.504360+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.06446","citing_title":"Method to study $CP$ violation in $B_s^0\\to K_S K^\\pm \\pi^\\mp$ decays","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7","json":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7.json","graph_json":"https://pith.science/api/pith-number/RY6OVYV5XNMPYXR7O2UOXIUWK7/graph.json","events_json":"https://pith.science/api/pith-number/RY6OVYV5XNMPYXR7O2UOXIUWK7/events.json","paper":"https://pith.science/paper/RY6OVYV5"},"agent_actions":{"view_html":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7","download_json":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7.json","view_paper":"https://pith.science/paper/RY6OVYV5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0905.3615&json=true","fetch_graph":"https://pith.science/api/pith-number/RY6OVYV5XNMPYXR7O2UOXIUWK7/graph.json","fetch_events":"https://pith.science/api/pith-number/RY6OVYV5XNMPYXR7O2UOXIUWK7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7/action/storage_attestation","attest_author":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7/action/author_attestation","sign_citation":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7/action/citation_signature","submit_replication":"https://pith.science/pith/RY6OVYV5XNMPYXR7O2UOXIUWK7/action/replication_record"}},"created_at":"2026-07-04T17:26:08.504360+00:00","updated_at":"2026-07-04T17:26:08.504360+00:00"}