{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:4GQ53HAV3YRD45MUVOPLBE6SHC","short_pith_number":"pith:4GQ53HAV","schema_version":"1.0","canonical_sha256":"e1a1dd9c15de223e7594ab9eb093d2388c67de57240897cb3bf67e331dac0eb8","source":{"kind":"arxiv","id":"1801.07975","version":7},"attestation_state":"computed","paper":{"title":"Removal Energies and Final State Interaction in Lepton Nucleus Scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"nucl-th","authors_text":"Arie Bodek, Tejin Cai","submitted_at":"2018-01-24T13:23:13Z","abstract_excerpt":"We investigate the binding energy parameters that should be used in modeling electron and neutrino scattering from nucleons bound in a nucleus within the framework of the impulse approximation. We discuss the relation between binding energy, missing energy, removal energy ($\\epsilon$), spectral functions and shell model energy levels and extract updated removal energy parameters from ee$^{\\prime}$p spectral function data. We address the difference in parameters for scattering from bound protons and neutrons. We also use inclusive e-A data to extract an empirical parameter $U_{FSI}( (\\vec q_3+\\"},"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":"1801.07975","kind":"arxiv","version":7},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-01-24T13:23:13Z","cross_cats_sorted":["hep-ex","hep-ph"],"title_canon_sha256":"2f24f8e43b6290efa603d0b748127f3e1beb8698d672e14e95a243589d6af1c9","abstract_canon_sha256":"7b5b96f486f68437446f6628030c8cc564f57797b9486a283f2dcacca0c67101"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:43.439957Z","signature_b64":"iRZoODqyyre8k7Od0iK0OEOkTRS79QHM3EzhCgDx//cBMrnVoG+74xY1QJcdTPjC5zJjVABwWNI9oigGlLodDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1a1dd9c15de223e7594ab9eb093d2388c67de57240897cb3bf67e331dac0eb8","last_reissued_at":"2026-05-17T23:44:43.439451Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:43.439451Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Removal Energies and Final State Interaction in Lepton Nucleus Scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"nucl-th","authors_text":"Arie Bodek, Tejin Cai","submitted_at":"2018-01-24T13:23:13Z","abstract_excerpt":"We investigate the binding energy parameters that should be used in modeling electron and neutrino scattering from nucleons bound in a nucleus within the framework of the impulse approximation. We discuss the relation between binding energy, missing energy, removal energy ($\\epsilon$), spectral functions and shell model energy levels and extract updated removal energy parameters from ee$^{\\prime}$p spectral function data. We address the difference in parameters for scattering from bound protons and neutrons. We also use inclusive e-A data to extract an empirical parameter $U_{FSI}( (\\vec q_3+\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.07975","kind":"arxiv","version":7},"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":"1801.07975","created_at":"2026-05-17T23:44:43.439535+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.07975v7","created_at":"2026-05-17T23:44:43.439535+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.07975","created_at":"2026-05-17T23:44:43.439535+00:00"},{"alias_kind":"pith_short_12","alias_value":"4GQ53HAV3YRD","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"4GQ53HAV3YRD45MU","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"4GQ53HAV","created_at":"2026-05-18T12:32:05.422762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.00745","citing_title":"Comparisons of triple-differential cross sections for quasielastic-like $\\nu_\\mu$-hydrocarbon interactions using $\\langle E_\\nu\\rangle \\sim$ 3~GeV versus $\\sim$ 6~GeV beams in MINERvA","ref_index":250,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC","json":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC.json","graph_json":"https://pith.science/api/pith-number/4GQ53HAV3YRD45MUVOPLBE6SHC/graph.json","events_json":"https://pith.science/api/pith-number/4GQ53HAV3YRD45MUVOPLBE6SHC/events.json","paper":"https://pith.science/paper/4GQ53HAV"},"agent_actions":{"view_html":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC","download_json":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC.json","view_paper":"https://pith.science/paper/4GQ53HAV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.07975&json=true","fetch_graph":"https://pith.science/api/pith-number/4GQ53HAV3YRD45MUVOPLBE6SHC/graph.json","fetch_events":"https://pith.science/api/pith-number/4GQ53HAV3YRD45MUVOPLBE6SHC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC/action/storage_attestation","attest_author":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC/action/author_attestation","sign_citation":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC/action/citation_signature","submit_replication":"https://pith.science/pith/4GQ53HAV3YRD45MUVOPLBE6SHC/action/replication_record"}},"created_at":"2026-05-17T23:44:43.439535+00:00","updated_at":"2026-05-17T23:44:43.439535+00:00"}