{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:NNKV2DGVGF2ZI6AZ5TKPO7SHVC","short_pith_number":"pith:NNKV2DGV","schema_version":"1.0","canonical_sha256":"6b555d0cd53175947819ecd4f77e47a8a32236d90e4cb30cb10ee4d2ecdd33db","source":{"kind":"arxiv","id":"hep-ph/9804352","version":1},"attestation_state":"computed","paper":{"title":"Low Q^2 Jet Production at HERA in Next-to-Leading Order QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Potter, G. Kramer","submitted_at":"1998-04-21T17:19:42Z","abstract_excerpt":"We present next-to-leading order calculations of one- and two-jet production in eP collisions at HERA for photon virtualities in the range 1<Q^2<100 GeV^2. Soft and collinear singularities are extracted using the phase space slicing method. Numerical results are presented for HERA conditions with the Snowmass jet definition. The transition between photoproduction and deep-inelastic scattering is investigated in detail. We compare two approaches, the usual deep-inelastic theory, where the virtual photon couples only directly to quarks and antiquarks, and the photoproduction approach, where the "},"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-ph/9804352","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-04-21T17:19:42Z","cross_cats_sorted":[],"title_canon_sha256":"a4e748045e383f54dcb6a10c937c2cc41aab23733149a5416dce34a4606ac245","abstract_canon_sha256":"6d1da024e96b8bcb6de335005c9977c7efecdb546fd8b5f6281034894fbdce19"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:37.307204Z","signature_b64":"4Lmq9AUd80dnbAz6WK5kKFrloP+p/oOpSmeORKHynu4yntZBoSKzOqHoQ4dBp2h2+OojSoi3SgbQz/CMuPxHCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6b555d0cd53175947819ecd4f77e47a8a32236d90e4cb30cb10ee4d2ecdd33db","last_reissued_at":"2026-05-18T04:17:37.306774Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:37.306774Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low Q^2 Jet Production at HERA in Next-to-Leading Order QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Potter, G. Kramer","submitted_at":"1998-04-21T17:19:42Z","abstract_excerpt":"We present next-to-leading order calculations of one- and two-jet production in eP collisions at HERA for photon virtualities in the range 1<Q^2<100 GeV^2. Soft and collinear singularities are extracted using the phase space slicing method. Numerical results are presented for HERA conditions with the Snowmass jet definition. The transition between photoproduction and deep-inelastic scattering is investigated in detail. We compare two approaches, the usual deep-inelastic theory, where the virtual photon couples only directly to quarks and antiquarks, and the photoproduction approach, where the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9804352","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":"hep-ph/9804352","created_at":"2026-05-18T04:17:37.306836+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9804352v1","created_at":"2026-05-18T04:17:37.306836+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9804352","created_at":"2026-05-18T04:17:37.306836+00:00"},{"alias_kind":"pith_short_12","alias_value":"NNKV2DGVGF2Z","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_16","alias_value":"NNKV2DGVGF2ZI6AZ","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_8","alias_value":"NNKV2DGV","created_at":"2026-05-18T12:25:49.038998+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/NNKV2DGVGF2ZI6AZ5TKPO7SHVC","json":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC.json","graph_json":"https://pith.science/api/pith-number/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/graph.json","events_json":"https://pith.science/api/pith-number/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/events.json","paper":"https://pith.science/paper/NNKV2DGV"},"agent_actions":{"view_html":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC","download_json":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC.json","view_paper":"https://pith.science/paper/NNKV2DGV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9804352&json=true","fetch_graph":"https://pith.science/api/pith-number/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/graph.json","fetch_events":"https://pith.science/api/pith-number/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/action/storage_attestation","attest_author":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/action/author_attestation","sign_citation":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/action/citation_signature","submit_replication":"https://pith.science/pith/NNKV2DGVGF2ZI6AZ5TKPO7SHVC/action/replication_record"}},"created_at":"2026-05-18T04:17:37.306836+00:00","updated_at":"2026-05-18T04:17:37.306836+00:00"}