{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:PZAYEQTX4UDX5U3R7NOCCF3OTZ","short_pith_number":"pith:PZAYEQTX","schema_version":"1.0","canonical_sha256":"7e41824277e5077ed371fb5c21176e9e686153b2c6684cd0ac44562695029c80","source":{"kind":"arxiv","id":"1202.1457","version":1},"attestation_state":"computed","paper":{"title":"Measurements of F_{2} and R=\\sigma_{L}/\\sigma_{T} on Nuclear Targets in the Nucleon Resonance Region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"Vahe Mamyan","submitted_at":"2012-02-07T16:31:43Z","abstract_excerpt":"Jefferson Lab Experiment E04-001 used the Rosenbluth technique to measure R=\\sigma_{L}/\\sigma_{T} and F_{2} on nuclear targets. This experiment was part of a multilab effort to investigate quark-hadron duality and the electromagnetic and weak structure of the nuclei in the nucleon resonance region. In addition to the studies of quark-hadron duality in electron scattering on nuclear targets, these data will be used as input form factors in future analysis of neutrino data which investigate quark-hadron duality of the nucleon and nuclear axial structure functions. An important goal of this exper"},"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":"1202.1457","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2012-02-07T16:31:43Z","cross_cats_sorted":[],"title_canon_sha256":"5c93f1fdd645c678c9037d03bb735bc0369a2748b3d55a5c45ea68d60ba3ebf0","abstract_canon_sha256":"f301ac9b9dfa5e2b0221ae6aae45a0420526214a60e0bc43ed59d05f42004755"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:02:53.316037Z","signature_b64":"jQWpOErnOqjnFPeX6nQGw2xW5dXQpwWOkij/hcSRfYkPKdy8gb1z/RCPFrPi6QBe4u4NTt9Sp4vRr+ObSAyuCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7e41824277e5077ed371fb5c21176e9e686153b2c6684cd0ac44562695029c80","last_reissued_at":"2026-05-18T04:02:53.315196Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:02:53.315196Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of F_{2} and R=\\sigma_{L}/\\sigma_{T} on Nuclear Targets in the Nucleon Resonance Region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"Vahe Mamyan","submitted_at":"2012-02-07T16:31:43Z","abstract_excerpt":"Jefferson Lab Experiment E04-001 used the Rosenbluth technique to measure R=\\sigma_{L}/\\sigma_{T} and F_{2} on nuclear targets. This experiment was part of a multilab effort to investigate quark-hadron duality and the electromagnetic and weak structure of the nuclei in the nucleon resonance region. In addition to the studies of quark-hadron duality in electron scattering on nuclear targets, these data will be used as input form factors in future analysis of neutrino data which investigate quark-hadron duality of the nucleon and nuclear axial structure functions. An important goal of this exper"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.1457","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":"1202.1457","created_at":"2026-05-18T04:02:53.315337+00:00"},{"alias_kind":"arxiv_version","alias_value":"1202.1457v1","created_at":"2026-05-18T04:02:53.315337+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.1457","created_at":"2026-05-18T04:02:53.315337+00:00"},{"alias_kind":"pith_short_12","alias_value":"PZAYEQTX4UDX","created_at":"2026-05-18T12:27:18.751474+00:00"},{"alias_kind":"pith_short_16","alias_value":"PZAYEQTX4UDX5U3R","created_at":"2026-05-18T12:27:18.751474+00:00"},{"alias_kind":"pith_short_8","alias_value":"PZAYEQTX","created_at":"2026-05-18T12:27:18.751474+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.13316","citing_title":"Investigation of Medium Modifications to $^{12}$C Structure Functions in the Resonance Region","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ","json":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ.json","graph_json":"https://pith.science/api/pith-number/PZAYEQTX4UDX5U3R7NOCCF3OTZ/graph.json","events_json":"https://pith.science/api/pith-number/PZAYEQTX4UDX5U3R7NOCCF3OTZ/events.json","paper":"https://pith.science/paper/PZAYEQTX"},"agent_actions":{"view_html":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ","download_json":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ.json","view_paper":"https://pith.science/paper/PZAYEQTX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1202.1457&json=true","fetch_graph":"https://pith.science/api/pith-number/PZAYEQTX4UDX5U3R7NOCCF3OTZ/graph.json","fetch_events":"https://pith.science/api/pith-number/PZAYEQTX4UDX5U3R7NOCCF3OTZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ/action/storage_attestation","attest_author":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ/action/author_attestation","sign_citation":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ/action/citation_signature","submit_replication":"https://pith.science/pith/PZAYEQTX4UDX5U3R7NOCCF3OTZ/action/replication_record"}},"created_at":"2026-05-18T04:02:53.315337+00:00","updated_at":"2026-05-18T04:02:53.315337+00:00"}