{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:KFVJPIZTUIVEQNQSBTONFDQOHF","short_pith_number":"pith:KFVJPIZT","schema_version":"1.0","canonical_sha256":"516a97a333a22a4836120cdcd28e0e3971667f2c98634b4c7978c27d44dc3e51","source":{"kind":"arxiv","id":"1901.05965","version":2},"attestation_state":"computed","paper":{"title":"A Monte Carlo global analysis of the Standard Model Effective Field Theory: the top quark sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Cen Zhang, Eleni Vryonidou, Emanuele R. Nocera, Emma Slade, Fabio Maltoni, Juan Rojo, Nathan P. Hartland","submitted_at":"2019-01-17T19:00:00Z","abstract_excerpt":"We present a novel framework for carrying out global analyses of the Standard Model Effective Field Theory (SMEFT) at dimension-six: SMEFiT. This approach is based on the Monte Carlo replica method for deriving a faithful estimate of the experimental and theoretical uncertainties and enables one to construct the probability distribution in the space of the SMEFT degrees of freedom. As a proof of concept of the SMEFiT methodology, we present a first study of the constraints on the SMEFT provided by top quark production measurements from the LHC. Our analysis includes more than 30 independent me"},"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":"1901.05965","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-01-17T19:00:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"ac6e96915cce2251462a6b6bc8d50c75a5fe404981ef23436fdd765e36515397","abstract_canon_sha256":"2f5171b8b69691ceb2b4c362447c4b4a8932709dd3b70f10ba1e1a032d53183d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:17.406252Z","signature_b64":"/qJ2arFPUgTAkqPLc/oAWSgK2aQSxxFcFeVwGPZSBfgsO6/Ic+m+9DBpzdWVIfSINXlCSjLfwP79lmvkMkfaBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"516a97a333a22a4836120cdcd28e0e3971667f2c98634b4c7978c27d44dc3e51","last_reissued_at":"2026-05-17T23:47:17.405594Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:17.405594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Monte Carlo global analysis of the Standard Model Effective Field Theory: the top quark sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Cen Zhang, Eleni Vryonidou, Emanuele R. Nocera, Emma Slade, Fabio Maltoni, Juan Rojo, Nathan P. Hartland","submitted_at":"2019-01-17T19:00:00Z","abstract_excerpt":"We present a novel framework for carrying out global analyses of the Standard Model Effective Field Theory (SMEFT) at dimension-six: SMEFiT. This approach is based on the Monte Carlo replica method for deriving a faithful estimate of the experimental and theoretical uncertainties and enables one to construct the probability distribution in the space of the SMEFT degrees of freedom. As a proof of concept of the SMEFiT methodology, we present a first study of the constraints on the SMEFT provided by top quark production measurements from the LHC. Our analysis includes more than 30 independent me"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.05965","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":"1901.05965","created_at":"2026-05-17T23:47:17.405694+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.05965v2","created_at":"2026-05-17T23:47:17.405694+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.05965","created_at":"2026-05-17T23:47:17.405694+00:00"},{"alias_kind":"pith_short_12","alias_value":"KFVJPIZTUIVE","created_at":"2026-05-18T12:33:21.387695+00:00"},{"alias_kind":"pith_short_16","alias_value":"KFVJPIZTUIVEQNQS","created_at":"2026-05-18T12:33:21.387695+00:00"},{"alias_kind":"pith_short_8","alias_value":"KFVJPIZT","created_at":"2026-05-18T12:33:21.387695+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":36,"is_internal_anchor":true},{"citing_arxiv_id":"2605.11747","citing_title":"SMEFT everywhere: a NLO study of $\\boldsymbol{pp \\to t\\bar{t}H}$ with decaying tops","ref_index":14,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16596","citing_title":"New Physics Reach through Precision at Future Colliders: a Multi-Pronged Approach","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF","json":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF.json","graph_json":"https://pith.science/api/pith-number/KFVJPIZTUIVEQNQSBTONFDQOHF/graph.json","events_json":"https://pith.science/api/pith-number/KFVJPIZTUIVEQNQSBTONFDQOHF/events.json","paper":"https://pith.science/paper/KFVJPIZT"},"agent_actions":{"view_html":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF","download_json":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF.json","view_paper":"https://pith.science/paper/KFVJPIZT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.05965&json=true","fetch_graph":"https://pith.science/api/pith-number/KFVJPIZTUIVEQNQSBTONFDQOHF/graph.json","fetch_events":"https://pith.science/api/pith-number/KFVJPIZTUIVEQNQSBTONFDQOHF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF/action/storage_attestation","attest_author":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF/action/author_attestation","sign_citation":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF/action/citation_signature","submit_replication":"https://pith.science/pith/KFVJPIZTUIVEQNQSBTONFDQOHF/action/replication_record"}},"created_at":"2026-05-17T23:47:17.405694+00:00","updated_at":"2026-05-17T23:47:17.405694+00:00"}