{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:5TYZFGNEJDY7C3BXNPT6A4KGPA","short_pith_number":"pith:5TYZFGNE","schema_version":"1.0","canonical_sha256":"ecf19299a448f1f16c376be7e0714678107df94b1eca08be8eda99dc9bf2dce3","source":{"kind":"arxiv","id":"1607.01749","version":1},"attestation_state":"computed","paper":{"title":"Z+jet production at NNLO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Gehrmann-De Ridder, A. Huss, E.W.N. Glover, T.A. Morgan, T. Gehrmann","submitted_at":"2016-07-06T19:16:34Z","abstract_excerpt":"We give a brief overview of our calculation of the next-to-next-to-leading order (NNLO) QCD corrections to Z+jet production in hadronic collisions. Phenomenological results are presented which comprise various differential distributions for 8 TeV proton-proton collisions. A significant reduction of the scale uncertainties is observed throughout as we move from NLO to NNLO. We further discuss how this calculation can be used to describe the inclusive Z-boson production at large transverse momentum. To this end, the theory prediction is compared to the measurements performed by the ATLAS and CMS"},"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":"1607.01749","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-07-06T19:16:34Z","cross_cats_sorted":[],"title_canon_sha256":"9e37f4177be1dd221a9cfaf78a93ab852b5fe1b092e926145a346360925ed920","abstract_canon_sha256":"bd5ea562681f2d394b6506363b0924cf3de80834f4fe45f07d21c59f1f836eb3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:25.578380Z","signature_b64":"+9uAZaFY1L9ab9Zk2oxNB/b5gX4DOq2CvmgerfwCQrSrEx3ZjJstk/Bmw/TMdhNXTR9Hk81kyEXUxytBeE82DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ecf19299a448f1f16c376be7e0714678107df94b1eca08be8eda99dc9bf2dce3","last_reissued_at":"2026-05-18T01:11:25.577823Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:25.577823Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Z+jet production at NNLO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Gehrmann-De Ridder, A. Huss, E.W.N. Glover, T.A. Morgan, T. Gehrmann","submitted_at":"2016-07-06T19:16:34Z","abstract_excerpt":"We give a brief overview of our calculation of the next-to-next-to-leading order (NNLO) QCD corrections to Z+jet production in hadronic collisions. Phenomenological results are presented which comprise various differential distributions for 8 TeV proton-proton collisions. A significant reduction of the scale uncertainties is observed throughout as we move from NLO to NNLO. We further discuss how this calculation can be used to describe the inclusive Z-boson production at large transverse momentum. To this end, the theory prediction is compared to the measurements performed by the ATLAS and CMS"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.01749","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":"1607.01749","created_at":"2026-05-18T01:11:25.577922+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.01749v1","created_at":"2026-05-18T01:11:25.577922+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.01749","created_at":"2026-05-18T01:11:25.577922+00:00"},{"alias_kind":"pith_short_12","alias_value":"5TYZFGNEJDY7","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"5TYZFGNEJDY7C3BX","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"5TYZFGNE","created_at":"2026-05-18T12:30:01.593930+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1912.10053","citing_title":"New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC","ref_index":169,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA","json":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA.json","graph_json":"https://pith.science/api/pith-number/5TYZFGNEJDY7C3BXNPT6A4KGPA/graph.json","events_json":"https://pith.science/api/pith-number/5TYZFGNEJDY7C3BXNPT6A4KGPA/events.json","paper":"https://pith.science/paper/5TYZFGNE"},"agent_actions":{"view_html":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA","download_json":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA.json","view_paper":"https://pith.science/paper/5TYZFGNE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.01749&json=true","fetch_graph":"https://pith.science/api/pith-number/5TYZFGNEJDY7C3BXNPT6A4KGPA/graph.json","fetch_events":"https://pith.science/api/pith-number/5TYZFGNEJDY7C3BXNPT6A4KGPA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA/action/storage_attestation","attest_author":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA/action/author_attestation","sign_citation":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA/action/citation_signature","submit_replication":"https://pith.science/pith/5TYZFGNEJDY7C3BXNPT6A4KGPA/action/replication_record"}},"created_at":"2026-05-18T01:11:25.577922+00:00","updated_at":"2026-05-18T01:11:25.577922+00:00"}