{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:W4GEFGCMI6QDCP6D5IYPWQ2LMQ","short_pith_number":"pith:W4GEFGCM","schema_version":"1.0","canonical_sha256":"b70c42984c47a0313fc3ea30fb434b642213465cbc44790331120bf474249ebf","source":{"kind":"arxiv","id":"1704.05009","version":1},"attestation_state":"computed","paper":{"title":"Measurement of the $e^+e^-\\to K^0_{\\scriptscriptstyle S}K^\\pm\\pi^{\\mp}\\pi^0$ and $K^0_{\\scriptscriptstyle S}K^\\pm\\pi^\\mp\\eta$ cross sections using initial-state radiation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The BABAR Collaboration","submitted_at":"2017-04-17T16:11:02Z","abstract_excerpt":"The processes $e^+e^-\\to K^0_{\\scriptscriptstyle S}K^\\pm\\pi^{\\mp}\\pi^0$ and $e^+e^-\\to K^0_{\\scriptscriptstyle S}K^\\pm\\pi^{\\mp}\\eta$ are studied over a continuum of energies from threshold to 4 GeV with the initial-state photon radiation method. Using 454 fb$^{-1}$ data collected with the BABAR detector at the SLAC PEP-II storage ring, the first measurements of the cross sections for these processes are obtained. The intermediate resonance structures from $K^{*0}(K\\pi)^0$, $K^{*}(892)^\\pm(K\\pi)^\\mp$ and $K^0_{\\scriptscriptstyle S}K^\\pm\\rho^{\\mp}$ are studied. The $J/\\psi$ is observed in all of"},"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":"1704.05009","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2017-04-17T16:11:02Z","cross_cats_sorted":[],"title_canon_sha256":"b2d052a677211aa1958c64503304bf6e56e32807081cf6a1eb430c474a9a8569","abstract_canon_sha256":"0f5514f71ad2729eef56393ea07c64fe04d3575e7cee0e014fecd66bcdb46f17"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:42:52.268335Z","signature_b64":"hznQIBAfjaR0/nZqLFJjX47I/JLHHPNdfGPDe+k7trQyh4GqusK7PPJQzSLBp4ZfGC3TkzurOKB51V5ldxnaCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b70c42984c47a0313fc3ea30fb434b642213465cbc44790331120bf474249ebf","last_reissued_at":"2026-05-18T00:42:52.267582Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:42:52.267582Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the $e^+e^-\\to K^0_{\\scriptscriptstyle S}K^\\pm\\pi^{\\mp}\\pi^0$ and $K^0_{\\scriptscriptstyle S}K^\\pm\\pi^\\mp\\eta$ cross sections using initial-state radiation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The BABAR Collaboration","submitted_at":"2017-04-17T16:11:02Z","abstract_excerpt":"The processes $e^+e^-\\to K^0_{\\scriptscriptstyle S}K^\\pm\\pi^{\\mp}\\pi^0$ and $e^+e^-\\to K^0_{\\scriptscriptstyle S}K^\\pm\\pi^{\\mp}\\eta$ are studied over a continuum of energies from threshold to 4 GeV with the initial-state photon radiation method. Using 454 fb$^{-1}$ data collected with the BABAR detector at the SLAC PEP-II storage ring, the first measurements of the cross sections for these processes are obtained. The intermediate resonance structures from $K^{*0}(K\\pi)^0$, $K^{*}(892)^\\pm(K\\pi)^\\mp$ and $K^0_{\\scriptscriptstyle S}K^\\pm\\rho^{\\mp}$ are studied. The $J/\\psi$ is observed in all of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.05009","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":"1704.05009","created_at":"2026-05-18T00:42:52.267710+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.05009v1","created_at":"2026-05-18T00:42:52.267710+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.05009","created_at":"2026-05-18T00:42:52.267710+00:00"},{"alias_kind":"pith_short_12","alias_value":"W4GEFGCMI6QD","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"W4GEFGCMI6QDCP6D","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"W4GEFGCM","created_at":"2026-05-18T12:31:49.984773+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2006.04822","citing_title":"The anomalous magnetic moment of the muon in the Standard Model","ref_index":78,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ","json":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ.json","graph_json":"https://pith.science/api/pith-number/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/graph.json","events_json":"https://pith.science/api/pith-number/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/events.json","paper":"https://pith.science/paper/W4GEFGCM"},"agent_actions":{"view_html":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ","download_json":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ.json","view_paper":"https://pith.science/paper/W4GEFGCM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.05009&json=true","fetch_graph":"https://pith.science/api/pith-number/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/graph.json","fetch_events":"https://pith.science/api/pith-number/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/action/storage_attestation","attest_author":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/action/author_attestation","sign_citation":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/action/citation_signature","submit_replication":"https://pith.science/pith/W4GEFGCMI6QDCP6D5IYPWQ2LMQ/action/replication_record"}},"created_at":"2026-05-18T00:42:52.267710+00:00","updated_at":"2026-05-18T00:42:52.267710+00:00"}