{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:BQRMU7URCSCQOSLJ7PRZUC6GO2","short_pith_number":"pith:BQRMU7UR","schema_version":"1.0","canonical_sha256":"0c22ca7e911485074969fbe39a0bc676b2c63efdd300d742da6eefdb6f994d91","source":{"kind":"arxiv","id":"hep-ph/0007192","version":2},"attestation_state":"computed","paper":{"title":"Geometric scaling for the total gamma^* p cross section in the low x region","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.M. Stasto, J. Kwiecinski, K. Golec-Biernat","submitted_at":"2000-07-18T18:28:32Z","abstract_excerpt":"We observe that the saturation model of deep inelastic scattering, which successfully describes inclusive and diffractive data at small x, predicts a geometric scaling of the total gamma^* p cross section in the region of small Bjorken variable x. The geometric scaling in this case means that the cross section is a function of only one dimensionless variable tau = Q^2 R_0^2(x), where the function R_0(x) (called saturation radius) decreases with decreasing x. We show that the experimental data from HERA in the region x<0.01 confirm the expectations of this scaling over a very broad region of Q^"},"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/0007192","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2000-07-18T18:28:32Z","cross_cats_sorted":[],"title_canon_sha256":"c1c654ea9c56db8f64443164dc45e41536ca2b56a13ef0b191b6d87088948fb6","abstract_canon_sha256":"ef272ffa3c9ae3d1ff11ad5b8141bd8157e2e3ff888d85b5b72a2d5eed7e96a4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:46.218758Z","signature_b64":"poH56vAy4fIS+vAHf/htDoa32wHm3bHhBwX/Qobh+1xbPJ+M43JNmcVhA1i7ebzw7XKg3NSDE+b5qO99fsi+Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0c22ca7e911485074969fbe39a0bc676b2c63efdd300d742da6eefdb6f994d91","last_reissued_at":"2026-07-04T15:20:46.218341Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:46.218341Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Geometric scaling for the total gamma^* p cross section in the low x region","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.M. Stasto, J. Kwiecinski, K. Golec-Biernat","submitted_at":"2000-07-18T18:28:32Z","abstract_excerpt":"We observe that the saturation model of deep inelastic scattering, which successfully describes inclusive and diffractive data at small x, predicts a geometric scaling of the total gamma^* p cross section in the region of small Bjorken variable x. The geometric scaling in this case means that the cross section is a function of only one dimensionless variable tau = Q^2 R_0^2(x), where the function R_0(x) (called saturation radius) decreases with decreasing x. We show that the experimental data from HERA in the region x<0.01 confirm the expectations of this scaling over a very broad region of Q^"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0007192","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-ph/0007192/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-ph/0007192","created_at":"2026-07-04T15:20:46.218407+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0007192v2","created_at":"2026-07-04T15:20:46.218407+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0007192","created_at":"2026-07-04T15:20:46.218407+00:00"},{"alias_kind":"pith_short_12","alias_value":"BQRMU7URCSCQ","created_at":"2026-07-04T15:20:46.218407+00:00"},{"alias_kind":"pith_short_16","alias_value":"BQRMU7URCSCQOSLJ","created_at":"2026-07-04T15:20:46.218407+00:00"},{"alias_kind":"pith_short_8","alias_value":"BQRMU7UR","created_at":"2026-07-04T15:20:46.218407+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2606.02108","citing_title":"Radial-flow fluctuations in the geometrical-scaling framework","ref_index":12,"is_internal_anchor":true},{"citing_arxiv_id":"2606.31754","citing_title":"Emergent Local Phase-Space Scaling in Small-x Gluon Evolution","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2605.27857","citing_title":"Multiplicity distributions in DIS for heavy nucleus","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15494","citing_title":"Forward hadron production in pp collisions at LHC energies from an event generator based on the color glass condensate framework","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2","json":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2.json","graph_json":"https://pith.science/api/pith-number/BQRMU7URCSCQOSLJ7PRZUC6GO2/graph.json","events_json":"https://pith.science/api/pith-number/BQRMU7URCSCQOSLJ7PRZUC6GO2/events.json","paper":"https://pith.science/paper/BQRMU7UR"},"agent_actions":{"view_html":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2","download_json":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2.json","view_paper":"https://pith.science/paper/BQRMU7UR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0007192&json=true","fetch_graph":"https://pith.science/api/pith-number/BQRMU7URCSCQOSLJ7PRZUC6GO2/graph.json","fetch_events":"https://pith.science/api/pith-number/BQRMU7URCSCQOSLJ7PRZUC6GO2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2/action/storage_attestation","attest_author":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2/action/author_attestation","sign_citation":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2/action/citation_signature","submit_replication":"https://pith.science/pith/BQRMU7URCSCQOSLJ7PRZUC6GO2/action/replication_record"}},"created_at":"2026-07-04T15:20:46.218407+00:00","updated_at":"2026-07-04T15:20:46.218407+00:00"}