{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:2HMKKH6RNFNCLLNYORQ4DRV37R","short_pith_number":"pith:2HMKKH6R","schema_version":"1.0","canonical_sha256":"d1d8a51fd1695a25adb87461c1c6bbfc6af211db4afdbab1fdb2191ec2baa16e","source":{"kind":"arxiv","id":"hep-ex/0611032","version":2},"attestation_state":"computed","paper":{"title":"chi_{cJ} Decays to h^+h^-h^0","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CLEO Collaboration, et al, S. Athar","submitted_at":"2006-11-17T13:40:30Z","abstract_excerpt":"Using a sample of 3 million psi(2S) decays recorded by the CLEO detector, we study three-body decays of the chi_c0, chi_c1, and chi_c2 produced in radiative decays of the psi(2S). We consider the final states pi+ pi- eta, K+ K- eta, p p-bar eta, pi+ pi- eta-prime, K+ K- pi0, p p-bar pi0, pi+ K- K0S, and K+ p-bar Lambda, measuring branching fractions or placing upper limits. For chi_c1 decays to pi+ pi- eta, K+ K- pi0, and pi+ K- K0S our observed samples are large enough to indicate the largest contributions to the substructure."},"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":"hep-ex/0611032","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2006-11-17T13:40:30Z","cross_cats_sorted":[],"title_canon_sha256":"a765ad6bad02ee1c8517b7efc8fcc93be3d2d6cdbdd5b34308f5d654999a1d84","abstract_canon_sha256":"ef2ee971a02f457be65d2006bb60bd0bba682a7118777eaa4d7bcca81415f699"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:24:30.466001Z","signature_b64":"mlbSnUeJCcTnrUrFFokYA1oPAMXjfMz2rDBwlooFecnLcuC4u8UDehS/U1sIalyEf7UdWZYUQ1/7fJwcpoIkBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1d8a51fd1695a25adb87461c1c6bbfc6af211db4afdbab1fdb2191ec2baa16e","last_reissued_at":"2026-05-18T03:24:30.465530Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:24:30.465530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"chi_{cJ} Decays to h^+h^-h^0","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CLEO Collaboration, et al, S. Athar","submitted_at":"2006-11-17T13:40:30Z","abstract_excerpt":"Using a sample of 3 million psi(2S) decays recorded by the CLEO detector, we study three-body decays of the chi_c0, chi_c1, and chi_c2 produced in radiative decays of the psi(2S). We consider the final states pi+ pi- eta, K+ K- eta, p p-bar eta, pi+ pi- eta-prime, K+ K- pi0, p p-bar pi0, pi+ K- K0S, and K+ p-bar Lambda, measuring branching fractions or placing upper limits. For chi_c1 decays to pi+ pi- eta, K+ K- pi0, and pi+ K- K0S our observed samples are large enough to indicate the largest contributions to the substructure."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0611032","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":"hep-ex/0611032","created_at":"2026-05-18T03:24:30.465604+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0611032v2","created_at":"2026-05-18T03:24:30.465604+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0611032","created_at":"2026-05-18T03:24:30.465604+00:00"},{"alias_kind":"pith_short_12","alias_value":"2HMKKH6RNFNC","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"2HMKKH6RNFNCLLNY","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"2HMKKH6R","created_at":"2026-05-18T12:25:53.939244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R","json":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R.json","graph_json":"https://pith.science/api/pith-number/2HMKKH6RNFNCLLNYORQ4DRV37R/graph.json","events_json":"https://pith.science/api/pith-number/2HMKKH6RNFNCLLNYORQ4DRV37R/events.json","paper":"https://pith.science/paper/2HMKKH6R"},"agent_actions":{"view_html":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R","download_json":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R.json","view_paper":"https://pith.science/paper/2HMKKH6R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0611032&json=true","fetch_graph":"https://pith.science/api/pith-number/2HMKKH6RNFNCLLNYORQ4DRV37R/graph.json","fetch_events":"https://pith.science/api/pith-number/2HMKKH6RNFNCLLNYORQ4DRV37R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R/action/storage_attestation","attest_author":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R/action/author_attestation","sign_citation":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R/action/citation_signature","submit_replication":"https://pith.science/pith/2HMKKH6RNFNCLLNYORQ4DRV37R/action/replication_record"}},"created_at":"2026-05-18T03:24:30.465604+00:00","updated_at":"2026-05-18T03:24:30.465604+00:00"}