{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:BCI2FQTPLZGBQDJQVRFVUNIL62","short_pith_number":"pith:BCI2FQTP","schema_version":"1.0","canonical_sha256":"0891a2c26f5e4c180d30ac4b5a350bf6b6246ed2257fcbd0c8d86a5be82a5787","source":{"kind":"arxiv","id":"1611.10100","version":2},"attestation_state":"computed","paper":{"title":"Dipole model analysis of highest precision HERA data, including very low $Q^2$'s","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Agnieszka Luszczak, Henri Kowalski","submitted_at":"2016-11-30T11:40:53Z","abstract_excerpt":"We analyse, within a dipole model, the final, inclusive HERA DIS cross section data in the low $x$ region, using fully correlated errors. We show, that these highest precision data are very well described within the dipole model framework starting from $Q^2$ values of 3.5 GeV$^2$ to the highest values of $Q^2 =$ 250 GeV$^2$."},"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":"1611.10100","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-30T11:40:53Z","cross_cats_sorted":[],"title_canon_sha256":"cffdb87c4a7a793e6ab3e38bed8daadb1b8007f03d3b9d263b017c337b8eee98","abstract_canon_sha256":"0986e1213af4d05fcbfdc0a17be3e728a58f57176443b148274f81ff04ce2fa4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:41.938723Z","signature_b64":"AH5vqtVkaXmWO8rjSRbSDKsgWRyqA1j7muDyDyX1ANTL3b30BQbmzKkjFhAervt6RJcXB5KZuuckrBeMvHPWDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0891a2c26f5e4c180d30ac4b5a350bf6b6246ed2257fcbd0c8d86a5be82a5787","last_reissued_at":"2026-05-18T00:51:41.938066Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:41.938066Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dipole model analysis of highest precision HERA data, including very low $Q^2$'s","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Agnieszka Luszczak, Henri Kowalski","submitted_at":"2016-11-30T11:40:53Z","abstract_excerpt":"We analyse, within a dipole model, the final, inclusive HERA DIS cross section data in the low $x$ region, using fully correlated errors. We show, that these highest precision data are very well described within the dipole model framework starting from $Q^2$ values of 3.5 GeV$^2$ to the highest values of $Q^2 =$ 250 GeV$^2$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.10100","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":""},"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":"1611.10100","created_at":"2026-05-18T00:51:41.938165+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.10100v2","created_at":"2026-05-18T00:51:41.938165+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.10100","created_at":"2026-05-18T00:51:41.938165+00:00"},{"alias_kind":"pith_short_12","alias_value":"BCI2FQTPLZGB","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_16","alias_value":"BCI2FQTPLZGBQDJQ","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_8","alias_value":"BCI2FQTP","created_at":"2026-05-18T12:30:07.202191+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/BCI2FQTPLZGBQDJQVRFVUNIL62","json":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62.json","graph_json":"https://pith.science/api/pith-number/BCI2FQTPLZGBQDJQVRFVUNIL62/graph.json","events_json":"https://pith.science/api/pith-number/BCI2FQTPLZGBQDJQVRFVUNIL62/events.json","paper":"https://pith.science/paper/BCI2FQTP"},"agent_actions":{"view_html":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62","download_json":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62.json","view_paper":"https://pith.science/paper/BCI2FQTP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.10100&json=true","fetch_graph":"https://pith.science/api/pith-number/BCI2FQTPLZGBQDJQVRFVUNIL62/graph.json","fetch_events":"https://pith.science/api/pith-number/BCI2FQTPLZGBQDJQVRFVUNIL62/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62/action/storage_attestation","attest_author":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62/action/author_attestation","sign_citation":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62/action/citation_signature","submit_replication":"https://pith.science/pith/BCI2FQTPLZGBQDJQVRFVUNIL62/action/replication_record"}},"created_at":"2026-05-18T00:51:41.938165+00:00","updated_at":"2026-05-18T00:51:41.938165+00:00"}