{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:SN4E6VR25TNNJJ3ALYT7KDS5VE","short_pith_number":"pith:SN4E6VR2","schema_version":"1.0","canonical_sha256":"93784f563aecdad4a7605e27f50e5da93a54fedb7beb554deee805faa543ec7e","source":{"kind":"arxiv","id":"hep-ex/0605105","version":1},"attestation_state":"computed","paper":{"title":"Measurements of the cross sections for $e^+e^- \\to {\\rm hadrons}$ at 3.650, 3.6648, 3.773 GeV and the branching fraction for $\\psi(3770)\\to {\\rm non-}D\\bar D$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"M. Ablikim et al. (BES Collaboration)","submitted_at":"2006-05-24T16:27:34Z","abstract_excerpt":"Using the BES-II detector at the BEPC Collider, we measured the lowest order cross sections and the $R$ values ($R=\\sigma^0_{e^+e^- \\to {\\rm hadrons}}/\\sigma^0_{e^+e^- \\to \\mu^+\\mu^-}$) for inclusive hadronic event production at the center-of-mass energies of 3.650 GeV, 3.6648 GeV and 3.773 GeV. The results lead to $\\bar R_{uds}=2.224\\pm 0.019\\pm 0.089$ which is the average of these measured at 3.650 GeV and 3.6648 GeV, and $R=3.793\\pm 0.037 \\pm 0.190$ at $\\sqrt{s}=3.773$ GeV. We determined the lowest order cross section for $\\psi(3770)$ production to be $\\sigma^{\\rm B}_{\\psi(3770)} = (9.575\\p"},"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/0605105","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2006-05-24T16:27:34Z","cross_cats_sorted":[],"title_canon_sha256":"ad132e0a3b88e16236b5c3ae82efe80f3c461f82d0452be5ff7e7eb53f19aab1","abstract_canon_sha256":"19c10a6748be87414acd32f19f3d2e9a0576399f118716b4c3598d3c4cb289a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:21.153527Z","signature_b64":"qAe/ul94n3DM23SlG92jykiWE7BJN+miCF4mXXYT8yQSvU8ZUy2FDBwxCXxsm1kk5QBZM8Slx6uI+bKkpJnUCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93784f563aecdad4a7605e27f50e5da93a54fedb7beb554deee805faa543ec7e","last_reissued_at":"2026-07-04T15:19:21.153130Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:21.153130Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of the cross sections for $e^+e^- \\to {\\rm hadrons}$ at 3.650, 3.6648, 3.773 GeV and the branching fraction for $\\psi(3770)\\to {\\rm non-}D\\bar D$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"M. Ablikim et al. (BES Collaboration)","submitted_at":"2006-05-24T16:27:34Z","abstract_excerpt":"Using the BES-II detector at the BEPC Collider, we measured the lowest order cross sections and the $R$ values ($R=\\sigma^0_{e^+e^- \\to {\\rm hadrons}}/\\sigma^0_{e^+e^- \\to \\mu^+\\mu^-}$) for inclusive hadronic event production at the center-of-mass energies of 3.650 GeV, 3.6648 GeV and 3.773 GeV. The results lead to $\\bar R_{uds}=2.224\\pm 0.019\\pm 0.089$ which is the average of these measured at 3.650 GeV and 3.6648 GeV, and $R=3.793\\pm 0.037 \\pm 0.190$ at $\\sqrt{s}=3.773$ GeV. We determined the lowest order cross section for $\\psi(3770)$ production to be $\\sigma^{\\rm B}_{\\psi(3770)} = (9.575\\p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0605105","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/hep-ex/0605105/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":"hep-ex/0605105","created_at":"2026-07-04T15:19:21.153195+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0605105v1","created_at":"2026-07-04T15:19:21.153195+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0605105","created_at":"2026-07-04T15:19:21.153195+00:00"},{"alias_kind":"pith_short_12","alias_value":"SN4E6VR25TNN","created_at":"2026-07-04T15:19:21.153195+00:00"},{"alias_kind":"pith_short_16","alias_value":"SN4E6VR25TNNJJ3A","created_at":"2026-07-04T15:19:21.153195+00:00"},{"alias_kind":"pith_short_8","alias_value":"SN4E6VR2","created_at":"2026-07-04T15:19:21.153195+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.10112","citing_title":"Calibrated correlation between heavy-quark masses and Hadronic Vacuum Polarization observables at the precision frontier","ref_index":63,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE","json":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE.json","graph_json":"https://pith.science/api/pith-number/SN4E6VR25TNNJJ3ALYT7KDS5VE/graph.json","events_json":"https://pith.science/api/pith-number/SN4E6VR25TNNJJ3ALYT7KDS5VE/events.json","paper":"https://pith.science/paper/SN4E6VR2"},"agent_actions":{"view_html":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE","download_json":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE.json","view_paper":"https://pith.science/paper/SN4E6VR2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0605105&json=true","fetch_graph":"https://pith.science/api/pith-number/SN4E6VR25TNNJJ3ALYT7KDS5VE/graph.json","fetch_events":"https://pith.science/api/pith-number/SN4E6VR25TNNJJ3ALYT7KDS5VE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE/action/storage_attestation","attest_author":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE/action/author_attestation","sign_citation":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE/action/citation_signature","submit_replication":"https://pith.science/pith/SN4E6VR25TNNJJ3ALYT7KDS5VE/action/replication_record"}},"created_at":"2026-07-04T15:19:21.153195+00:00","updated_at":"2026-07-04T15:19:21.153195+00:00"}