{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:RZFBLWG55OFMF3ODUYQGZUMASZ","short_pith_number":"pith:RZFBLWG5","schema_version":"1.0","canonical_sha256":"8e4a15d8ddeb8ac2edc3a6206cd180966c8a62f5db41af1f462726f231607ba4","source":{"kind":"arxiv","id":"0904.2296","version":1},"attestation_state":"computed","paper":{"title":"New measurement of charge asymmetry $x{F}_3$ from HERA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Laurent Schoeffel","submitted_at":"2009-04-15T12:38:54Z","abstract_excerpt":"After presenting the recent measurements of neutral current cross section in DIS at HERA, we explain the effect of the $\\gamma-Z_0$ interference at the electro-weak scale, visible on these data. Then, the beam charge difference $x{F}_3$ is measured and the interference itself is extracted. Results are discussed in the context of perturbative QCD."},"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":"0904.2296","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-04-15T12:38:54Z","cross_cats_sorted":[],"title_canon_sha256":"02c801da4729ffeeab0168b0d16280a72e03771b457ecd35b8375eb778f014e7","abstract_canon_sha256":"188d6069aecbf0ccce2e17948d8fdb40768bb65349d7e1c3d8da1263afa4a1e1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:14:00.243538Z","signature_b64":"D59jbcS1J+yJxHNSohxWN39AsSDSgF3N1Lq9Rz5jtGuMWfsn2yj1fDG0Fqv1h3dPJZUkCIXziRgTHSGWI3PJAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e4a15d8ddeb8ac2edc3a6206cd180966c8a62f5db41af1f462726f231607ba4","last_reissued_at":"2026-05-18T02:14:00.242802Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:14:00.242802Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New measurement of charge asymmetry $x{F}_3$ from HERA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Laurent Schoeffel","submitted_at":"2009-04-15T12:38:54Z","abstract_excerpt":"After presenting the recent measurements of neutral current cross section in DIS at HERA, we explain the effect of the $\\gamma-Z_0$ interference at the electro-weak scale, visible on these data. Then, the beam charge difference $x{F}_3$ is measured and the interference itself is extracted. Results are discussed in the context of perturbative QCD."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.2296","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":"0904.2296","created_at":"2026-05-18T02:14:00.242931+00:00"},{"alias_kind":"arxiv_version","alias_value":"0904.2296v1","created_at":"2026-05-18T02:14:00.242931+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.2296","created_at":"2026-05-18T02:14:00.242931+00:00"},{"alias_kind":"pith_short_12","alias_value":"RZFBLWG55OFM","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"RZFBLWG55OFMF3OD","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"RZFBLWG5","created_at":"2026-05-18T12:26:01.383474+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/RZFBLWG55OFMF3ODUYQGZUMASZ","json":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ.json","graph_json":"https://pith.science/api/pith-number/RZFBLWG55OFMF3ODUYQGZUMASZ/graph.json","events_json":"https://pith.science/api/pith-number/RZFBLWG55OFMF3ODUYQGZUMASZ/events.json","paper":"https://pith.science/paper/RZFBLWG5"},"agent_actions":{"view_html":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ","download_json":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ.json","view_paper":"https://pith.science/paper/RZFBLWG5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0904.2296&json=true","fetch_graph":"https://pith.science/api/pith-number/RZFBLWG55OFMF3ODUYQGZUMASZ/graph.json","fetch_events":"https://pith.science/api/pith-number/RZFBLWG55OFMF3ODUYQGZUMASZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ/action/storage_attestation","attest_author":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ/action/author_attestation","sign_citation":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ/action/citation_signature","submit_replication":"https://pith.science/pith/RZFBLWG55OFMF3ODUYQGZUMASZ/action/replication_record"}},"created_at":"2026-05-18T02:14:00.242931+00:00","updated_at":"2026-05-18T02:14:00.242931+00:00"}