{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:JVJ7BKQEFGK3FXNQKWB5IWBHPY","short_pith_number":"pith:JVJ7BKQE","schema_version":"1.0","canonical_sha256":"4d53f0aa042995b2ddb05583d458277e367d5da253e3a9a5dbb0d65d1a3aaa9f","source":{"kind":"arxiv","id":"1111.3636","version":2},"attestation_state":"computed","paper":{"title":"Amplitude analysis and measurement of the time-dependent CP asymmetry of $B^0 \\to K_0^S K_0^S K_0^S$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al., The BABAR Collaboration: J. P. Lees","submitted_at":"2011-11-15T20:55:09Z","abstract_excerpt":"We present the first results on the Dalitz-plot structure and improved measurements of the time-dependent CP-violation parameters of the process $B^0 \\rightarrow K^0_S K^0_S K^0_S$ obtained using $468\\times10^{6}$ $B\\bar{B}$ decays collected with the BABAR detector at the PEP-II asymmetric-energy $B$ factory at SLAC. The Dalitz-plot structure is probed by a time-integrated amplitude analysis that does not distinguish between $B^0$ and $\\bar{B}^0$ decays. We measure the total inclusive branching fraction ${\\cal B}($B^0$ \\rightarrow K^0_S K^0_S K^0_S)=\\rm (6.19 \\pm 0.48 \\pm 0.15 \\pm 0.12)\\times "},"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":"1111.3636","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-11-15T20:55:09Z","cross_cats_sorted":[],"title_canon_sha256":"9af49138df6c68ad7c9d52cc2e042bfd67804d757965905ac48c4ce106a35175","abstract_canon_sha256":"7e2abc9298c5e2f480cb0736ddc719b8cd50e2ed3b559dd2e81621989c9048f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:57:44.014450Z","signature_b64":"DaoGsM52DkxJNNydrODC71rmFSna6X/ymZjXD7Nd2fLKOqXt4GV2ylv5PkgLPggagbhysH3fTZwx0qZB7QnWCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d53f0aa042995b2ddb05583d458277e367d5da253e3a9a5dbb0d65d1a3aaa9f","last_reissued_at":"2026-07-04T23:57:44.013858Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:57:44.013858Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Amplitude analysis and measurement of the time-dependent CP asymmetry of $B^0 \\to K_0^S K_0^S K_0^S$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al., The BABAR Collaboration: J. P. Lees","submitted_at":"2011-11-15T20:55:09Z","abstract_excerpt":"We present the first results on the Dalitz-plot structure and improved measurements of the time-dependent CP-violation parameters of the process $B^0 \\rightarrow K^0_S K^0_S K^0_S$ obtained using $468\\times10^{6}$ $B\\bar{B}$ decays collected with the BABAR detector at the PEP-II asymmetric-energy $B$ factory at SLAC. The Dalitz-plot structure is probed by a time-integrated amplitude analysis that does not distinguish between $B^0$ and $\\bar{B}^0$ decays. We measure the total inclusive branching fraction ${\\cal B}($B^0$ \\rightarrow K^0_S K^0_S K^0_S)=\\rm (6.19 \\pm 0.48 \\pm 0.15 \\pm 0.12)\\times "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.3636","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/1111.3636/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":"1111.3636","created_at":"2026-07-04T23:57:44.013935+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.3636v2","created_at":"2026-07-04T23:57:44.013935+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.3636","created_at":"2026-07-04T23:57:44.013935+00:00"},{"alias_kind":"pith_short_12","alias_value":"JVJ7BKQEFGK3","created_at":"2026-07-04T23:57:44.013935+00:00"},{"alias_kind":"pith_short_16","alias_value":"JVJ7BKQEFGK3FXNQ","created_at":"2026-07-04T23:57:44.013935+00:00"},{"alias_kind":"pith_short_8","alias_value":"JVJ7BKQE","created_at":"2026-07-04T23:57:44.013935+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.18907","citing_title":"Quasi-Two-Body $B\\to P (K^+K^-, \\pi^+\\pi^-)$ Decays with $f_0(980)$ Resonance","ref_index":36,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY","json":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY.json","graph_json":"https://pith.science/api/pith-number/JVJ7BKQEFGK3FXNQKWB5IWBHPY/graph.json","events_json":"https://pith.science/api/pith-number/JVJ7BKQEFGK3FXNQKWB5IWBHPY/events.json","paper":"https://pith.science/paper/JVJ7BKQE"},"agent_actions":{"view_html":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY","download_json":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY.json","view_paper":"https://pith.science/paper/JVJ7BKQE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.3636&json=true","fetch_graph":"https://pith.science/api/pith-number/JVJ7BKQEFGK3FXNQKWB5IWBHPY/graph.json","fetch_events":"https://pith.science/api/pith-number/JVJ7BKQEFGK3FXNQKWB5IWBHPY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY/action/storage_attestation","attest_author":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY/action/author_attestation","sign_citation":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY/action/citation_signature","submit_replication":"https://pith.science/pith/JVJ7BKQEFGK3FXNQKWB5IWBHPY/action/replication_record"}},"created_at":"2026-07-04T23:57:44.013935+00:00","updated_at":"2026-07-04T23:57:44.013935+00:00"}