{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:3ZFQBB3IDDHLK5TTT7DX54CZDA","short_pith_number":"pith:3ZFQBB3I","schema_version":"1.0","canonical_sha256":"de4b00876818ceb576739fc77ef059182ca0733f7235eb2d2dc2b609d2ce69ae","source":{"kind":"arxiv","id":"1308.5694","version":1},"attestation_state":"computed","paper":{"title":"Strangeness Vector and Axial-Vector Form Factors of the Nucleon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dennis Trujillo, Stephen Pate","submitted_at":"2013-08-26T20:21:50Z","abstract_excerpt":"A revised global fit of electroweak $ep$ and $\\nu p$ elastic scattering data has been performed, with the goal of determining the strange quark contribution to the vector and axial-vector form factors of the nucleon in the momentum-transfer range $0<Q^2<1$ GeV$^2$. The two vector (electric and magnetic) form factors $G_E^s(Q^2)$ and $G_M^s(Q^2)$ are strongly constrained by $ep$ elastic scattering data, while the major source of information on the axial-vector form factor $G_A^s(Q^2)$ is $\\nu p$ scattering data. Combining the two kinds of data into a single global fit makes possible additional "},"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":"1308.5694","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-26T20:21:50Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3fc6b1a06f5c08c72f3dc955c2b7ca4e8647d276151eceba2bf156e9c2ec2868","abstract_canon_sha256":"5c186dbbad19c45c8f34b14fef841df6ca89619b05c44ff6e8f9603cd3f3fa90"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:52.401434Z","signature_b64":"S7TJ8k1r/wrHxhU82AjH/RlXJ03hORLoCjKXdaruPQ+ShfSa9o3ZLJN2tgObGOvXj6NgVdAiKHVux1LJ0OpLCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de4b00876818ceb576739fc77ef059182ca0733f7235eb2d2dc2b609d2ce69ae","last_reissued_at":"2026-05-18T02:35:52.400837Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:52.400837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strangeness Vector and Axial-Vector Form Factors of the Nucleon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dennis Trujillo, Stephen Pate","submitted_at":"2013-08-26T20:21:50Z","abstract_excerpt":"A revised global fit of electroweak $ep$ and $\\nu p$ elastic scattering data has been performed, with the goal of determining the strange quark contribution to the vector and axial-vector form factors of the nucleon in the momentum-transfer range $0<Q^2<1$ GeV$^2$. The two vector (electric and magnetic) form factors $G_E^s(Q^2)$ and $G_M^s(Q^2)$ are strongly constrained by $ep$ elastic scattering data, while the major source of information on the axial-vector form factor $G_A^s(Q^2)$ is $\\nu p$ scattering data. Combining the two kinds of data into a single global fit makes possible additional "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.5694","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":"1308.5694","created_at":"2026-05-18T02:35:52.400955+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.5694v1","created_at":"2026-05-18T02:35:52.400955+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.5694","created_at":"2026-05-18T02:35:52.400955+00:00"},{"alias_kind":"pith_short_12","alias_value":"3ZFQBB3IDDHL","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_16","alias_value":"3ZFQBB3IDDHLK5TT","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_8","alias_value":"3ZFQBB3I","created_at":"2026-05-18T12:27:32.513160+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/3ZFQBB3IDDHLK5TTT7DX54CZDA","json":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA.json","graph_json":"https://pith.science/api/pith-number/3ZFQBB3IDDHLK5TTT7DX54CZDA/graph.json","events_json":"https://pith.science/api/pith-number/3ZFQBB3IDDHLK5TTT7DX54CZDA/events.json","paper":"https://pith.science/paper/3ZFQBB3I"},"agent_actions":{"view_html":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA","download_json":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA.json","view_paper":"https://pith.science/paper/3ZFQBB3I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.5694&json=true","fetch_graph":"https://pith.science/api/pith-number/3ZFQBB3IDDHLK5TTT7DX54CZDA/graph.json","fetch_events":"https://pith.science/api/pith-number/3ZFQBB3IDDHLK5TTT7DX54CZDA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA/action/storage_attestation","attest_author":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA/action/author_attestation","sign_citation":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA/action/citation_signature","submit_replication":"https://pith.science/pith/3ZFQBB3IDDHLK5TTT7DX54CZDA/action/replication_record"}},"created_at":"2026-05-18T02:35:52.400955+00:00","updated_at":"2026-05-18T02:35:52.400955+00:00"}