{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:SO32DWMEJL7HHFI2E55N3XS47M","short_pith_number":"pith:SO32DWME","schema_version":"1.0","canonical_sha256":"93b7a1d9844afe73951a277addde5cfb3cc325ea25aadfb5248c41dd61eb8d8e","source":{"kind":"arxiv","id":"hep-ex/0603026","version":1},"attestation_state":"computed","paper":{"title":"Search for the non-D\\barD Decay psi(3770) --> K_S^0 K_L^0","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CLEO Collaboration, D. Cronin-Hennessy, et al","submitted_at":"2006-03-13T15:15:31Z","abstract_excerpt":"Using the current world's largest data sample of psi(3770) decays, we present results of a search for the non-DDbar decay psi(3770) -> KsKl. We find no signal, and obtain an upper limit of Sigma(psi(3770) -> KsKl) < 0.07 pb at 90% confidence level (CL). Our result tests a theoretical prediction for the upper bound on B(psi(3770) -> KsKl) based on a charmonia-mixing model."},"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/0603026","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2006-03-13T15:15:31Z","cross_cats_sorted":[],"title_canon_sha256":"872da44d68b623022d33d9de6891d156c08241c991e43369fb29a69910735886","abstract_canon_sha256":"bb775b844edf9be06d0b4731fb43fbf3430e7708cb2f0591178a6eac0845a00a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:20.970654Z","signature_b64":"mNvzQ+O495j6NcyNLnsUX+zFVfzeBB2EjHDOsubeROy7cNCMEfqA9OvlUB9iqqjcYULHcOLfcWc72j4xv0jiCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93b7a1d9844afe73951a277addde5cfb3cc325ea25aadfb5248c41dd61eb8d8e","last_reissued_at":"2026-05-18T02:37:20.970238Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:20.970238Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for the non-D\\barD Decay psi(3770) --> K_S^0 K_L^0","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CLEO Collaboration, D. Cronin-Hennessy, et al","submitted_at":"2006-03-13T15:15:31Z","abstract_excerpt":"Using the current world's largest data sample of psi(3770) decays, we present results of a search for the non-DDbar decay psi(3770) -> KsKl. We find no signal, and obtain an upper limit of Sigma(psi(3770) -> KsKl) < 0.07 pb at 90% confidence level (CL). Our result tests a theoretical prediction for the upper bound on B(psi(3770) -> KsKl) based on a charmonia-mixing model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0603026","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":""},"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/0603026","created_at":"2026-05-18T02:37:20.970291+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0603026v1","created_at":"2026-05-18T02:37:20.970291+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0603026","created_at":"2026-05-18T02:37:20.970291+00:00"},{"alias_kind":"pith_short_12","alias_value":"SO32DWMEJL7H","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"SO32DWMEJL7HHFI2","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"SO32DWME","created_at":"2026-05-18T12:25:54.717736+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/SO32DWMEJL7HHFI2E55N3XS47M","json":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M.json","graph_json":"https://pith.science/api/pith-number/SO32DWMEJL7HHFI2E55N3XS47M/graph.json","events_json":"https://pith.science/api/pith-number/SO32DWMEJL7HHFI2E55N3XS47M/events.json","paper":"https://pith.science/paper/SO32DWME"},"agent_actions":{"view_html":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M","download_json":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M.json","view_paper":"https://pith.science/paper/SO32DWME","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0603026&json=true","fetch_graph":"https://pith.science/api/pith-number/SO32DWMEJL7HHFI2E55N3XS47M/graph.json","fetch_events":"https://pith.science/api/pith-number/SO32DWMEJL7HHFI2E55N3XS47M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M/action/storage_attestation","attest_author":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M/action/author_attestation","sign_citation":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M/action/citation_signature","submit_replication":"https://pith.science/pith/SO32DWMEJL7HHFI2E55N3XS47M/action/replication_record"}},"created_at":"2026-05-18T02:37:20.970291+00:00","updated_at":"2026-05-18T02:37:20.970291+00:00"}