{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:Y62I4MUXE7S6XJ4ZGPSYUPL554","short_pith_number":"pith:Y62I4MUX","schema_version":"1.0","canonical_sha256":"c7b48e329727e5eba79933e58a3d7def2320c11f04487ce4430da2879a94e28d","source":{"kind":"arxiv","id":"1611.08121","version":2},"attestation_state":"computed","paper":{"title":"Impact Factor for Exclusive Diffractive Dijet Production with NLO Accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. V. Grabovsky, L. Szymanowski, R.Boussarie, S. Wallon","submitted_at":"2016-11-24T09:55:28Z","abstract_excerpt":"Relying on the shockwave approach, we present the main steps of the computation of the impact factor for the exclusive diffractive photo- or electro- production of a forward dijet with NLO accuracy. We provide details of the cancellation mechanisms for all the divergences which appear in the intermediate results."},"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":"1611.08121","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-24T09:55:28Z","cross_cats_sorted":[],"title_canon_sha256":"7af95a014fadbec161bcdccc0e9b96b8674de786a995daa648877b879110b76e","abstract_canon_sha256":"4b4d330ae92507e32358dc29a71406d8d47f91e5db5ac8e10640e562eb0094c3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:20.298454Z","signature_b64":"Q2rGSUoGtNsRbP5/DSUT9WovKCdEWSAaHEm/fa5a+dTZ2jIAXFzaMsDMbKeTaCrxKkd2blsWljSPWtd/c/3sBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7b48e329727e5eba79933e58a3d7def2320c11f04487ce4430da2879a94e28d","last_reissued_at":"2026-05-18T00:47:20.297688Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:20.297688Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Impact Factor for Exclusive Diffractive Dijet Production with NLO Accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. V. Grabovsky, L. Szymanowski, R.Boussarie, S. Wallon","submitted_at":"2016-11-24T09:55:28Z","abstract_excerpt":"Relying on the shockwave approach, we present the main steps of the computation of the impact factor for the exclusive diffractive photo- or electro- production of a forward dijet with NLO accuracy. We provide details of the cancellation mechanisms for all the divergences which appear in the intermediate results."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.08121","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":"1611.08121","created_at":"2026-05-18T00:47:20.297816+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.08121v2","created_at":"2026-05-18T00:47:20.297816+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.08121","created_at":"2026-05-18T00:47:20.297816+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y62I4MUXE7S6","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y62I4MUXE7S6XJ4Z","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y62I4MUX","created_at":"2026-05-18T12:30:53.716459+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/Y62I4MUXE7S6XJ4ZGPSYUPL554","json":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554.json","graph_json":"https://pith.science/api/pith-number/Y62I4MUXE7S6XJ4ZGPSYUPL554/graph.json","events_json":"https://pith.science/api/pith-number/Y62I4MUXE7S6XJ4ZGPSYUPL554/events.json","paper":"https://pith.science/paper/Y62I4MUX"},"agent_actions":{"view_html":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554","download_json":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554.json","view_paper":"https://pith.science/paper/Y62I4MUX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.08121&json=true","fetch_graph":"https://pith.science/api/pith-number/Y62I4MUXE7S6XJ4ZGPSYUPL554/graph.json","fetch_events":"https://pith.science/api/pith-number/Y62I4MUXE7S6XJ4ZGPSYUPL554/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554/action/storage_attestation","attest_author":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554/action/author_attestation","sign_citation":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554/action/citation_signature","submit_replication":"https://pith.science/pith/Y62I4MUXE7S6XJ4ZGPSYUPL554/action/replication_record"}},"created_at":"2026-05-18T00:47:20.297816+00:00","updated_at":"2026-05-18T00:47:20.297816+00:00"}