{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:RT3NBFQV6WM7QSCSATEJ5XUOOB","short_pith_number":"pith:RT3NBFQV","schema_version":"1.0","canonical_sha256":"8cf6d09615f599f8485204c89ede8e705dca6b72cef18a77463e3e7a292bd233","source":{"kind":"arxiv","id":"1604.06444","version":2},"attestation_state":"computed","paper":{"title":"On the Validity of the Effective Field Theory Approach to SM Precision Tests","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Adam Falkowski, Christophe Grojean, Florian Goertz, Francesco Riva, Roberto Contino","submitted_at":"2016-04-21T19:54:52Z","abstract_excerpt":"We discuss the conditions for an effective field theory (EFT) to give an adequate low-energy description of an underlying physics beyond the Standard Model (SM). Starting from the EFT where the SM is extended by dimension-6 operators, experimental data can be used without further assumptions to measure (or set limits on) the EFT parameters. The interpretation of these results requires instead a set of broad assumptions (e.g. power counting rules) on the UV dynamics. This allows one to establish, in a bottom-up approach, the validity range of the EFT description, and to assess the error associa"},"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":"1604.06444","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-04-21T19:54:52Z","cross_cats_sorted":[],"title_canon_sha256":"90c843b894951feea319d5cdf92b0a838721dae8b660aa8fee305401e6dd06ec","abstract_canon_sha256":"655dfc499f6b1fb77d3b1b0c6d8d19bf1a2c1b6077f98a1c64857b0dc75af428"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:12.425049Z","signature_b64":"3XU7YS5xG26YKqE/rZfSSHYjIxNEfddp5OhVtR1eoEXwfWCKkyHjTmjx0bPKALDosvtzg4QRGXl/U+mdpyVxAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8cf6d09615f599f8485204c89ede8e705dca6b72cef18a77463e3e7a292bd233","last_reissued_at":"2026-05-18T01:05:12.424299Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:12.424299Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the Validity of the Effective Field Theory Approach to SM Precision Tests","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Adam Falkowski, Christophe Grojean, Florian Goertz, Francesco Riva, Roberto Contino","submitted_at":"2016-04-21T19:54:52Z","abstract_excerpt":"We discuss the conditions for an effective field theory (EFT) to give an adequate low-energy description of an underlying physics beyond the Standard Model (SM). Starting from the EFT where the SM is extended by dimension-6 operators, experimental data can be used without further assumptions to measure (or set limits on) the EFT parameters. The interpretation of these results requires instead a set of broad assumptions (e.g. power counting rules) on the UV dynamics. This allows one to establish, in a bottom-up approach, the validity range of the EFT description, and to assess the error associa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06444","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":"1604.06444","created_at":"2026-05-18T01:05:12.424427+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.06444v2","created_at":"2026-05-18T01:05:12.424427+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06444","created_at":"2026-05-18T01:05:12.424427+00:00"},{"alias_kind":"pith_short_12","alias_value":"RT3NBFQV6WM7","created_at":"2026-05-18T12:30:41.710351+00:00"},{"alias_kind":"pith_short_16","alias_value":"RT3NBFQV6WM7QSCS","created_at":"2026-05-18T12:30:41.710351+00:00"},{"alias_kind":"pith_short_8","alias_value":"RT3NBFQV","created_at":"2026-05-18T12:30:41.710351+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.23159","citing_title":"Muonphilic asymmetric dark matter at a future muon collider","ref_index":43,"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":71,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08688","citing_title":"Probing Higgs and Top Interactions through the Muon Lens at multi-TeV Muon Colliders","ref_index":71,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB","json":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB.json","graph_json":"https://pith.science/api/pith-number/RT3NBFQV6WM7QSCSATEJ5XUOOB/graph.json","events_json":"https://pith.science/api/pith-number/RT3NBFQV6WM7QSCSATEJ5XUOOB/events.json","paper":"https://pith.science/paper/RT3NBFQV"},"agent_actions":{"view_html":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB","download_json":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB.json","view_paper":"https://pith.science/paper/RT3NBFQV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.06444&json=true","fetch_graph":"https://pith.science/api/pith-number/RT3NBFQV6WM7QSCSATEJ5XUOOB/graph.json","fetch_events":"https://pith.science/api/pith-number/RT3NBFQV6WM7QSCSATEJ5XUOOB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB/action/storage_attestation","attest_author":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB/action/author_attestation","sign_citation":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB/action/citation_signature","submit_replication":"https://pith.science/pith/RT3NBFQV6WM7QSCSATEJ5XUOOB/action/replication_record"}},"created_at":"2026-05-18T01:05:12.424427+00:00","updated_at":"2026-05-18T01:05:12.424427+00:00"}