{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UMLFKP4SOOFZGZGYLML452DTXJ","short_pith_number":"pith:UMLFKP4S","schema_version":"1.0","canonical_sha256":"a316553f92738b9364d85b17cee873ba7245e0082901737bba731d272d3b001f","source":{"kind":"arxiv","id":"1409.8545","version":1},"attestation_state":"computed","paper":{"title":"Effective Spectral Function for Quasielastic Scattering on Nuclei from Deuterium to Lead","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Bodek, B. Coopersmith, M. E. Christy","submitted_at":"2014-09-30T13:46:08Z","abstract_excerpt":"Spectral functions do not fully describe quasielastic electron and neutrino scattering from nuclei because they only model the initial state. Final state interactions distort the shape of the differential cross section at the peak and increase the cross section at the tails of the distribution. We show that the kinematic distributions predicted by the $\\psi'$ superscaling formalism can be well described with a modified {\\it {effective spectral function}} (ESF). By construction, models using ESF in combination with the transverse enhancement contribution correctly predict electron QE scattering"},"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":"1409.8545","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-09-30T13:46:08Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex"],"title_canon_sha256":"75467c2c409cf078967797c375c61a7dce45c823786f7015867373a207cc45c1","abstract_canon_sha256":"ee78e24f81569e7c259dd07f0b5f1b8e4975d7e15c6757973d525ee4ba4cbe8a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:09.840436Z","signature_b64":"G6swurhZJ1SMENXDXbvu6dGSaN4RPUEzBWJuPzuHIdQqmeMtJtcxbN1YDmqjnDYuEFye+gwPc4zvUNRE+OYHCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a316553f92738b9364d85b17cee873ba7245e0082901737bba731d272d3b001f","last_reissued_at":"2026-05-18T01:13:09.839926Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:09.839926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Spectral Function for Quasielastic Scattering on Nuclei from Deuterium to Lead","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Bodek, B. Coopersmith, M. E. Christy","submitted_at":"2014-09-30T13:46:08Z","abstract_excerpt":"Spectral functions do not fully describe quasielastic electron and neutrino scattering from nuclei because they only model the initial state. Final state interactions distort the shape of the differential cross section at the peak and increase the cross section at the tails of the distribution. We show that the kinematic distributions predicted by the $\\psi'$ superscaling formalism can be well described with a modified {\\it {effective spectral function}} (ESF). By construction, models using ESF in combination with the transverse enhancement contribution correctly predict electron QE scattering"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.8545","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":"1409.8545","created_at":"2026-05-18T01:13:09.839985+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.8545v1","created_at":"2026-05-18T01:13:09.839985+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.8545","created_at":"2026-05-18T01:13:09.839985+00:00"},{"alias_kind":"pith_short_12","alias_value":"UMLFKP4SOOFZ","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UMLFKP4SOOFZGZGY","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UMLFKP4S","created_at":"2026-05-18T12:28:52.271510+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/UMLFKP4SOOFZGZGYLML452DTXJ","json":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ.json","graph_json":"https://pith.science/api/pith-number/UMLFKP4SOOFZGZGYLML452DTXJ/graph.json","events_json":"https://pith.science/api/pith-number/UMLFKP4SOOFZGZGYLML452DTXJ/events.json","paper":"https://pith.science/paper/UMLFKP4S"},"agent_actions":{"view_html":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ","download_json":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ.json","view_paper":"https://pith.science/paper/UMLFKP4S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.8545&json=true","fetch_graph":"https://pith.science/api/pith-number/UMLFKP4SOOFZGZGYLML452DTXJ/graph.json","fetch_events":"https://pith.science/api/pith-number/UMLFKP4SOOFZGZGYLML452DTXJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ/action/storage_attestation","attest_author":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ/action/author_attestation","sign_citation":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ/action/citation_signature","submit_replication":"https://pith.science/pith/UMLFKP4SOOFZGZGYLML452DTXJ/action/replication_record"}},"created_at":"2026-05-18T01:13:09.839985+00:00","updated_at":"2026-05-18T01:13:09.839985+00:00"}