{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:EHBE7QEWN6Q74BBAJUXDHCV24S","short_pith_number":"pith:EHBE7QEW","schema_version":"1.0","canonical_sha256":"21c24fc0966fa1fe04204d2e338abae48a5083ada13bfb9199131eb89b095fa9","source":{"kind":"arxiv","id":"nucl-th/0603014","version":1},"attestation_state":"computed","paper":{"title":"Target mass corrections revisited","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"F. M. Steffens, W. Melnitchouk","submitted_at":"2006-03-06T14:48:40Z","abstract_excerpt":"We propose a new implementation of target mass corrections to nucleon structure functions which, unlike existing treatments, has the correct kinematic threshold behavior at finite Q^2 in the x -> 1 limit. We illustrate the differences between the new approach and existing prescriptions by considering specific examples for the F_2 and F_L structure functions, and discuss the broader implications of our results, which call into question the notion of universal parton distribution at finite Q^2."},"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":"nucl-th/0603014","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-03-06T14:48:40Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6774e18f97879191193c8482646c8683846cf2dd6a13d31df857bcc3f8cd4547","abstract_canon_sha256":"15facb1bb739685496c95e0ecd0b86247550976bc41e19a4f86b5c126e48e155"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:07.879452Z","signature_b64":"zEH7f1Hti0OhV1bwdmlq0kTnfaFDLe2CL5R7I9gEjaZhr2F/2Xy0KlWxQcthxp3kWsepe4ZuRoQKhSNag/g5DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"21c24fc0966fa1fe04204d2e338abae48a5083ada13bfb9199131eb89b095fa9","last_reissued_at":"2026-05-18T02:35:07.879021Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:07.879021Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Target mass corrections revisited","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"F. M. Steffens, W. Melnitchouk","submitted_at":"2006-03-06T14:48:40Z","abstract_excerpt":"We propose a new implementation of target mass corrections to nucleon structure functions which, unlike existing treatments, has the correct kinematic threshold behavior at finite Q^2 in the x -> 1 limit. We illustrate the differences between the new approach and existing prescriptions by considering specific examples for the F_2 and F_L structure functions, and discuss the broader implications of our results, which call into question the notion of universal parton distribution at finite Q^2."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0603014","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":"nucl-th/0603014","created_at":"2026-05-18T02:35:07.879085+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0603014v1","created_at":"2026-05-18T02:35:07.879085+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0603014","created_at":"2026-05-18T02:35:07.879085+00:00"},{"alias_kind":"pith_short_12","alias_value":"EHBE7QEWN6Q7","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"EHBE7QEWN6Q74BBA","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"EHBE7QEW","created_at":"2026-05-18T12:25:53.939244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.00666","citing_title":"Stability of parton distributions at high $x$: impact of nuclear and power corrections","ref_index":87,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S","json":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S.json","graph_json":"https://pith.science/api/pith-number/EHBE7QEWN6Q74BBAJUXDHCV24S/graph.json","events_json":"https://pith.science/api/pith-number/EHBE7QEWN6Q74BBAJUXDHCV24S/events.json","paper":"https://pith.science/paper/EHBE7QEW"},"agent_actions":{"view_html":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S","download_json":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S.json","view_paper":"https://pith.science/paper/EHBE7QEW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0603014&json=true","fetch_graph":"https://pith.science/api/pith-number/EHBE7QEWN6Q74BBAJUXDHCV24S/graph.json","fetch_events":"https://pith.science/api/pith-number/EHBE7QEWN6Q74BBAJUXDHCV24S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S/action/storage_attestation","attest_author":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S/action/author_attestation","sign_citation":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S/action/citation_signature","submit_replication":"https://pith.science/pith/EHBE7QEWN6Q74BBAJUXDHCV24S/action/replication_record"}},"created_at":"2026-05-18T02:35:07.879085+00:00","updated_at":"2026-05-18T02:35:07.879085+00:00"}