{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:GAUHSWNX3YJOXZSEGCAEOGHZ4P","short_pith_number":"pith:GAUHSWNX","schema_version":"1.0","canonical_sha256":"30287959b7de12ebe64430804718f9e3d54d3dd3b1ddf765918cf1991d53ada4","source":{"kind":"arxiv","id":"2106.05337","version":3},"attestation_state":"computed","paper":{"title":"Dilepton production in the SMEFT at $\\mathcal O(1/\\Lambda^4)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Emanuele Mereghetti, Frank Petriello, Radja Boughezal","submitted_at":"2021-06-09T18:51:00Z","abstract_excerpt":"We study the inclusion of $\\mathcal O(1/\\Lambda^4)$ effects in the Standard Model Effective Field Theory in fits to the current Drell-Yan data at the LHC. Our analysis includes the full set of dimension-6 and dimension-8 operators contributing to the dilepton process, and is performed to next-to-leading-order in the QCD coupling constant at both $\\mathcal O(1/\\Lambda^2)$ and $\\mathcal O(1/\\Lambda^4)$. We find that the inclusion of dimension-6 squared terms and certain dimension-8 operators has significant effects on fits to the current data. Neglecting them leads to bounds on dimension-6 opera"},"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":"2106.05337","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-06-09T18:51:00Z","cross_cats_sorted":[],"title_canon_sha256":"badbd1edd538735da9ce6872c367c948850e4959e34f43a457c6d50a8f511d67","abstract_canon_sha256":"15cb8f2c3cb5f529bf6f337c17209ab4b42e11838d53056560170b7484c70837"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:21:26.020581Z","signature_b64":"NgYO1PmEVupSIuZ/TGng/7uOvfNYKiu7m+WS+ApICEbY/TJCcDMf/yZLz2xZBraEBjplvnFluxHyaZWGA5gqCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30287959b7de12ebe64430804718f9e3d54d3dd3b1ddf765918cf1991d53ada4","last_reissued_at":"2026-07-05T04:21:26.020075Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:21:26.020075Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dilepton production in the SMEFT at $\\mathcal O(1/\\Lambda^4)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Emanuele Mereghetti, Frank Petriello, Radja Boughezal","submitted_at":"2021-06-09T18:51:00Z","abstract_excerpt":"We study the inclusion of $\\mathcal O(1/\\Lambda^4)$ effects in the Standard Model Effective Field Theory in fits to the current Drell-Yan data at the LHC. Our analysis includes the full set of dimension-6 and dimension-8 operators contributing to the dilepton process, and is performed to next-to-leading-order in the QCD coupling constant at both $\\mathcal O(1/\\Lambda^2)$ and $\\mathcal O(1/\\Lambda^4)$. We find that the inclusion of dimension-6 squared terms and certain dimension-8 operators has significant effects on fits to the current data. Neglecting them leads to bounds on dimension-6 opera"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.05337","kind":"arxiv","version":3},"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/2106.05337/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":"2106.05337","created_at":"2026-07-05T04:21:26.020135+00:00"},{"alias_kind":"arxiv_version","alias_value":"2106.05337v3","created_at":"2026-07-05T04:21:26.020135+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.05337","created_at":"2026-07-05T04:21:26.020135+00:00"},{"alias_kind":"pith_short_12","alias_value":"GAUHSWNX3YJO","created_at":"2026-07-05T04:21:26.020135+00:00"},{"alias_kind":"pith_short_16","alias_value":"GAUHSWNX3YJOXZSE","created_at":"2026-07-05T04:21:26.020135+00:00"},{"alias_kind":"pith_short_8","alias_value":"GAUHSWNX","created_at":"2026-07-05T04:21:26.020135+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2408.07255","citing_title":"Dihadron azimuthal asymmetry and light-quark dipole moments at the Electron-Ion Collider","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15262","citing_title":"USMEFT as a tool for discovery of universal new physics at high luminosity LHC","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2508.08516","citing_title":"Nucleon Energy Correlators as a Probe of Light-Quark Dipole Operators at the Electron-Ion Collider","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":47,"is_internal_anchor":false},{"citing_arxiv_id":"2604.00107","citing_title":"Full positivity bounds for anomalous quartic gauge couplings in SMEFT","ref_index":27,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P","json":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P.json","graph_json":"https://pith.science/api/pith-number/GAUHSWNX3YJOXZSEGCAEOGHZ4P/graph.json","events_json":"https://pith.science/api/pith-number/GAUHSWNX3YJOXZSEGCAEOGHZ4P/events.json","paper":"https://pith.science/paper/GAUHSWNX"},"agent_actions":{"view_html":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P","download_json":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P.json","view_paper":"https://pith.science/paper/GAUHSWNX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2106.05337&json=true","fetch_graph":"https://pith.science/api/pith-number/GAUHSWNX3YJOXZSEGCAEOGHZ4P/graph.json","fetch_events":"https://pith.science/api/pith-number/GAUHSWNX3YJOXZSEGCAEOGHZ4P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P/action/storage_attestation","attest_author":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P/action/author_attestation","sign_citation":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P/action/citation_signature","submit_replication":"https://pith.science/pith/GAUHSWNX3YJOXZSEGCAEOGHZ4P/action/replication_record"}},"created_at":"2026-07-05T04:21:26.020135+00:00","updated_at":"2026-07-05T04:21:26.020135+00:00"}