{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:OZW5KGVUPEVXQG3NWRJYQHCFNO","short_pith_number":"pith:OZW5KGVU","schema_version":"1.0","canonical_sha256":"766dd51ab4792b781b6db453881c456b84cbaf1be64263aab7832ec5836796fd","source":{"kind":"arxiv","id":"1502.01683","version":1},"attestation_state":"computed","paper":{"title":"Diffractive Dijet Production with a Leading Proton in ep Collisions at HERA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"H1 Collaboration","submitted_at":"2015-02-05T19:12:57Z","abstract_excerpt":"The cross section of the diffractive process e^+p -> e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 <2 GeV^2 and in deep-inelastic scattering with 4 GeV^2<Q^2<80 GeV^2. The results are compared to next-to-leading order QCD calculations based on diffractive parton distribution functions as extracted from measurements of inclusive cross sections in diffractive deep-inelasti"},"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":"1502.01683","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2015-02-05T19:12:57Z","cross_cats_sorted":[],"title_canon_sha256":"5a8df777bfa6fda3da95706b70c3cdad0a17ad16ba3c7801a41a509b7e96051a","abstract_canon_sha256":"212bc40e407008f403d7d4e70048cebb0f36e2a4feb7fcfefd1da3c238050926"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:27:51.542367Z","signature_b64":"GTwmjvPLRwBc5aF/pLzJAXPJe4UJfKCBtXDV+f2HlsCp0Obf+nbo9L5gZqZnaGNRXJ3TiZFVeGvV4V6JYRktDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"766dd51ab4792b781b6db453881c456b84cbaf1be64263aab7832ec5836796fd","last_reissued_at":"2026-05-18T02:27:51.541838Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:27:51.541838Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Diffractive Dijet Production with a Leading Proton in ep Collisions at HERA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"H1 Collaboration","submitted_at":"2015-02-05T19:12:57Z","abstract_excerpt":"The cross section of the diffractive process e^+p -> e^+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q^2 <2 GeV^2 and in deep-inelastic scattering with 4 GeV^2<Q^2<80 GeV^2. The results are compared to next-to-leading order QCD calculations based on diffractive parton distribution functions as extracted from measurements of inclusive cross sections in diffractive deep-inelasti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.01683","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":"1502.01683","created_at":"2026-05-18T02:27:51.541930+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.01683v1","created_at":"2026-05-18T02:27:51.541930+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.01683","created_at":"2026-05-18T02:27:51.541930+00:00"},{"alias_kind":"pith_short_12","alias_value":"OZW5KGVUPEVX","created_at":"2026-05-18T12:29:34.919912+00:00"},{"alias_kind":"pith_short_16","alias_value":"OZW5KGVUPEVXQG3N","created_at":"2026-05-18T12:29:34.919912+00:00"},{"alias_kind":"pith_short_8","alias_value":"OZW5KGVU","created_at":"2026-05-18T12:29:34.919912+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2203.11601","citing_title":"A comprehensive guide to the physics and usage of PYTHIA 8.3","ref_index":271,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24435","citing_title":"Measurement of jet photoproduction in ultra-peripheral Pb+Pb collisions without nuclear breakup at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20559","citing_title":"Observation of impact parameter dependent modifications of nuclear parton distributions in photonuclear Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","ref_index":27,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO","json":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO.json","graph_json":"https://pith.science/api/pith-number/OZW5KGVUPEVXQG3NWRJYQHCFNO/graph.json","events_json":"https://pith.science/api/pith-number/OZW5KGVUPEVXQG3NWRJYQHCFNO/events.json","paper":"https://pith.science/paper/OZW5KGVU"},"agent_actions":{"view_html":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO","download_json":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO.json","view_paper":"https://pith.science/paper/OZW5KGVU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.01683&json=true","fetch_graph":"https://pith.science/api/pith-number/OZW5KGVUPEVXQG3NWRJYQHCFNO/graph.json","fetch_events":"https://pith.science/api/pith-number/OZW5KGVUPEVXQG3NWRJYQHCFNO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO/action/storage_attestation","attest_author":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO/action/author_attestation","sign_citation":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO/action/citation_signature","submit_replication":"https://pith.science/pith/OZW5KGVUPEVXQG3NWRJYQHCFNO/action/replication_record"}},"created_at":"2026-05-18T02:27:51.541930+00:00","updated_at":"2026-05-18T02:27:51.541930+00:00"}