{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:K5E4T4L3LN5MET6ENOIYFFMQZ4","short_pith_number":"pith:K5E4T4L3","schema_version":"1.0","canonical_sha256":"5749c9f17b5b7ac24fc46b91829590cf13829e17cfbb0b73ab252582ca4e6220","source":{"kind":"arxiv","id":"hep-lat/0507007","version":2},"attestation_state":"computed","paper":{"title":"Deep-inelastic scattering and the operator product expansion in lattice QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"C.-J. David Lin, William Detmold","submitted_at":"2005-07-08T23:14:27Z","abstract_excerpt":"We discuss the determination of deep-inelastic hadron structure in lattice QCD. By using a fictitious heavy quark, direct calculations of the Compton scattering tensor can be performed in Euclidean space that allow the extraction of the moments of structure functions. This overcomes issues of operator mixing and renormalisation that have so far prohibited lattice computations of higher moments. This approach is especially suitable for the study of the twist-two contributions to isovector quark distributions, which is practical with current computing resources. While we focus on the isovector u"},"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":"hep-lat/0507007","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-07-08T23:14:27Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"e2fca31b2afef1bd5f182ec5544c9b5575ebbe717cb1c2bd114e797fb39d0718","abstract_canon_sha256":"33da7fe0b9151a8bb41361e0372e12a20214cd0c23c8b1605017f794f67093d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:24.423431Z","signature_b64":"ozyqKc8gI4tkwKfIbGvTl0HorukWLKmGRRNoGy46g1I4qClyvA82JNE6Ma132YyLypOASHvlOn1gnDsqoOBHAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5749c9f17b5b7ac24fc46b91829590cf13829e17cfbb0b73ab252582ca4e6220","last_reissued_at":"2026-07-04T15:22:24.423059Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:24.423059Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deep-inelastic scattering and the operator product expansion in lattice QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"C.-J. David Lin, William Detmold","submitted_at":"2005-07-08T23:14:27Z","abstract_excerpt":"We discuss the determination of deep-inelastic hadron structure in lattice QCD. By using a fictitious heavy quark, direct calculations of the Compton scattering tensor can be performed in Euclidean space that allow the extraction of the moments of structure functions. This overcomes issues of operator mixing and renormalisation that have so far prohibited lattice computations of higher moments. This approach is especially suitable for the study of the twist-two contributions to isovector quark distributions, which is practical with current computing resources. While we focus on the isovector u"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0507007","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0507007/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-lat/0507007","created_at":"2026-07-04T15:22:24.423114+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0507007v2","created_at":"2026-07-04T15:22:24.423114+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0507007","created_at":"2026-07-04T15:22:24.423114+00:00"},{"alias_kind":"pith_short_12","alias_value":"K5E4T4L3LN5M","created_at":"2026-07-04T15:22:24.423114+00:00"},{"alias_kind":"pith_short_16","alias_value":"K5E4T4L3LN5MET6E","created_at":"2026-07-04T15:22:24.423114+00:00"},{"alias_kind":"pith_short_8","alias_value":"K5E4T4L3","created_at":"2026-07-04T15:22:24.423114+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2606.02447","citing_title":"Kinematic enhancement for nucleon interpolators","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2605.30193","citing_title":"Mellin Moments of the Unpolarized Gluon PDF in the Proton from Nonlocal Operators in Lattice QCD","ref_index":18,"is_internal_anchor":true},{"citing_arxiv_id":"1907.09827","citing_title":"Parton distribution functions of $\\Delta^+$ on the lattice","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2311.04206","citing_title":"Elastic and resonance structures of the nucleon from hadronic tensor in lattice QCD: implications for neutrino-nucleon scattering and hadron physics","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2603.28604","citing_title":"Hadron Structure from lattice QCD in the context of the Electron-Ion Collider","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12373","citing_title":"Quasi Parton Distribution Functions in Covariant Quark Models","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4","json":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4.json","graph_json":"https://pith.science/api/pith-number/K5E4T4L3LN5MET6ENOIYFFMQZ4/graph.json","events_json":"https://pith.science/api/pith-number/K5E4T4L3LN5MET6ENOIYFFMQZ4/events.json","paper":"https://pith.science/paper/K5E4T4L3"},"agent_actions":{"view_html":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4","download_json":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4.json","view_paper":"https://pith.science/paper/K5E4T4L3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0507007&json=true","fetch_graph":"https://pith.science/api/pith-number/K5E4T4L3LN5MET6ENOIYFFMQZ4/graph.json","fetch_events":"https://pith.science/api/pith-number/K5E4T4L3LN5MET6ENOIYFFMQZ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4/action/storage_attestation","attest_author":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4/action/author_attestation","sign_citation":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4/action/citation_signature","submit_replication":"https://pith.science/pith/K5E4T4L3LN5MET6ENOIYFFMQZ4/action/replication_record"}},"created_at":"2026-07-04T15:22:24.423114+00:00","updated_at":"2026-07-04T15:22:24.423114+00:00"}