{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:QRV66WNPN2SJKN45A6K55U4JAI","short_pith_number":"pith:QRV66WNP","schema_version":"1.0","canonical_sha256":"846bef59af6ea495379d0795ded389023f7e0c7e779bf08b2467c5e2641ab8fe","source":{"kind":"arxiv","id":"1411.0669","version":3},"attestation_state":"computed","paper":{"title":"Model-independent precision constraints on dimension-6 operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Adam Falkowski, Francesco Riva","submitted_at":"2014-11-03T21:00:04Z","abstract_excerpt":"We discuss electroweak precision constraints on dimension-6 operators in the effective theory beyond the standard model. We identify the combinations of these operators that are constrained by the pole observables (the W and Z masses and on-shell decays) and by the W boson pair production. To this end, we define a set of effective couplings of W and Z bosons to fermions and to itself, which capture the effects of new physics corrections. This formalism clarifies which operators are constrained by which observable, independently of the adopted basis of operators. We obtain numerical constraints"},"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":"1411.0669","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-11-03T21:00:04Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"44aee148c8678840de8445a75e6295ed35bda5912a6afa033456151d7494981b","abstract_canon_sha256":"e6b305b9cc1ec2c6ccc13598e7d602ec60066ac90830a03124118e93b55c4bee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:35.733207Z","signature_b64":"lFQrJZDCQuGxnNIG7HrgJnzohah9usIWw6CvHEuPy2rqmJfBupW4rM0xUlcP0ZSvDAFE+kjlzFi+FzkgjYSJAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"846bef59af6ea495379d0795ded389023f7e0c7e779bf08b2467c5e2641ab8fe","last_reissued_at":"2026-05-18T01:41:35.732616Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:35.732616Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Model-independent precision constraints on dimension-6 operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Adam Falkowski, Francesco Riva","submitted_at":"2014-11-03T21:00:04Z","abstract_excerpt":"We discuss electroweak precision constraints on dimension-6 operators in the effective theory beyond the standard model. We identify the combinations of these operators that are constrained by the pole observables (the W and Z masses and on-shell decays) and by the W boson pair production. To this end, we define a set of effective couplings of W and Z bosons to fermions and to itself, which capture the effects of new physics corrections. This formalism clarifies which operators are constrained by which observable, independently of the adopted basis of operators. We obtain numerical constraints"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.0669","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":""},"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":"1411.0669","created_at":"2026-05-18T01:41:35.732690+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.0669v3","created_at":"2026-05-18T01:41:35.732690+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.0669","created_at":"2026-05-18T01:41:35.732690+00:00"},{"alias_kind":"pith_short_12","alias_value":"QRV66WNPN2SJ","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"QRV66WNPN2SJKN45","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"QRV66WNP","created_at":"2026-05-18T12:28:46.137349+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.07651","citing_title":"An EWPD SMEFT likelihood for the LHC -- and how to improve it with measurements of W and Z boson properties","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2605.08433","citing_title":"Electroweak Restoration: SMEFT and HEFT","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21670","citing_title":"Effective field theory interpretation of ATLAS measurements involving the Higgs boson, electroweak bosons and the top quark","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14274","citing_title":"The Spurion Massive EFT (SMEFT)","ref_index":4,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI","json":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI.json","graph_json":"https://pith.science/api/pith-number/QRV66WNPN2SJKN45A6K55U4JAI/graph.json","events_json":"https://pith.science/api/pith-number/QRV66WNPN2SJKN45A6K55U4JAI/events.json","paper":"https://pith.science/paper/QRV66WNP"},"agent_actions":{"view_html":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI","download_json":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI.json","view_paper":"https://pith.science/paper/QRV66WNP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.0669&json=true","fetch_graph":"https://pith.science/api/pith-number/QRV66WNPN2SJKN45A6K55U4JAI/graph.json","fetch_events":"https://pith.science/api/pith-number/QRV66WNPN2SJKN45A6K55U4JAI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI/action/storage_attestation","attest_author":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI/action/author_attestation","sign_citation":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI/action/citation_signature","submit_replication":"https://pith.science/pith/QRV66WNPN2SJKN45A6K55U4JAI/action/replication_record"}},"created_at":"2026-05-18T01:41:35.732690+00:00","updated_at":"2026-05-18T01:41:35.732690+00:00"}