{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:4HZK3CUJJ6HREKYLDZ4XGCMDQJ","short_pith_number":"pith:4HZK3CUJ","schema_version":"1.0","canonical_sha256":"e1f2ad8a894f8f122b0b1e79730983826bdde07a9ee76e188c0b0ca31b5217c7","source":{"kind":"arxiv","id":"2303.12781","version":1},"attestation_state":"computed","paper":{"title":"Drell-Yan lepton-pair production: $q_T$ resummation at approximate N$^4$LL+N$^4$LO accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giancarlo Ferrera, Leandro Cieri, Stefano Camarda","submitted_at":"2023-03-22T17:51:32Z","abstract_excerpt":"We consider Drell-Yan lepton pairs produced in hadronic collisions. We present high-accuracy QCD predictions for the transverse-momentum ($q_T$) distribution and fiducial cross sections in the small $q_T$ region. We resum to all perturbative orders the logarithmically enhanced contributions up to the next-to-next-to-next-to-next-to-leading logarithmic (N$^4$LL) accuracy and we include the hard-virtual coefficient at the next-to-next-to-next-to-leading order (N$^3$LO) (i.e. $\\mathcal{O}(\\alpha_S^3)$) with an approximation of the N$^4$LO coefficients. The massive axial-vector and vector contribu"},"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":"2303.12781","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-03-22T17:51:32Z","cross_cats_sorted":[],"title_canon_sha256":"05e1c0d7168cc2777038b15d85502ee812485ee279560fff901f396b2726da6b","abstract_canon_sha256":"9c5b22467e19bd7c8cac4039bf107f33c3dcca9964caa2662398c85048338f14"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:53:45.019677Z","signature_b64":"gwVhhKJiGzZUhY95YIC8sfp0bmMO3DP2OZ8x3c4jN3Hz14hnIq8owSSOXIDfehX8qkC1WSwrZ0XI/p+P+j8TCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1f2ad8a894f8f122b0b1e79730983826bdde07a9ee76e188c0b0ca31b5217c7","last_reissued_at":"2026-07-05T05:53:45.019281Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:53:45.019281Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Drell-Yan lepton-pair production: $q_T$ resummation at approximate N$^4$LL+N$^4$LO accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giancarlo Ferrera, Leandro Cieri, Stefano Camarda","submitted_at":"2023-03-22T17:51:32Z","abstract_excerpt":"We consider Drell-Yan lepton pairs produced in hadronic collisions. We present high-accuracy QCD predictions for the transverse-momentum ($q_T$) distribution and fiducial cross sections in the small $q_T$ region. We resum to all perturbative orders the logarithmically enhanced contributions up to the next-to-next-to-next-to-next-to-leading logarithmic (N$^4$LL) accuracy and we include the hard-virtual coefficient at the next-to-next-to-next-to-leading order (N$^3$LO) (i.e. $\\mathcal{O}(\\alpha_S^3)$) with an approximation of the N$^4$LO coefficients. The massive axial-vector and vector contribu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.12781","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2303.12781/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":"2303.12781","created_at":"2026-07-05T05:53:45.019340+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.12781v1","created_at":"2026-07-05T05:53:45.019340+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.12781","created_at":"2026-07-05T05:53:45.019340+00:00"},{"alias_kind":"pith_short_12","alias_value":"4HZK3CUJJ6HR","created_at":"2026-07-05T05:53:45.019340+00:00"},{"alias_kind":"pith_short_16","alias_value":"4HZK3CUJJ6HREKYL","created_at":"2026-07-05T05:53:45.019340+00:00"},{"alias_kind":"pith_short_8","alias_value":"4HZK3CUJ","created_at":"2026-07-05T05:53:45.019340+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.13759","citing_title":"Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","ref_index":62,"is_internal_anchor":false},{"citing_arxiv_id":"2510.07397","citing_title":"Slepton pair production at next-to-leading power","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ","json":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ.json","graph_json":"https://pith.science/api/pith-number/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/graph.json","events_json":"https://pith.science/api/pith-number/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/events.json","paper":"https://pith.science/paper/4HZK3CUJ"},"agent_actions":{"view_html":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ","download_json":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ.json","view_paper":"https://pith.science/paper/4HZK3CUJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.12781&json=true","fetch_graph":"https://pith.science/api/pith-number/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/graph.json","fetch_events":"https://pith.science/api/pith-number/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/action/storage_attestation","attest_author":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/action/author_attestation","sign_citation":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/action/citation_signature","submit_replication":"https://pith.science/pith/4HZK3CUJJ6HREKYLDZ4XGCMDQJ/action/replication_record"}},"created_at":"2026-07-05T05:53:45.019340+00:00","updated_at":"2026-07-05T05:53:45.019340+00:00"}