{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:KSGDBAGGRZZWVLYC6XDR6BCMJF","short_pith_number":"pith:KSGDBAGG","schema_version":"1.0","canonical_sha256":"548c3080c68e736aaf02f5c71f044c4955279b73464d90db863905eff87914ac","source":{"kind":"arxiv","id":"1904.03204","version":1},"attestation_state":"computed","paper":{"title":"SmeftFR -- Feynman rules generator for the Standard Model Effective Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Dedes, J. Rosiek, K. Suxho, L. Trifyllis, M. Paraskevas","submitted_at":"2019-04-05T18:00:32Z","abstract_excerpt":"We present SmeftFR, a Mathematica package designed to generate the Feynman rules for the Standard Model Effective Field Theory (SMEFT) including the complete set of gauge invariant operators up to dimension~6. Feynman rules are generated with the use of FeynRules package, directly in the physical (mass eigenstates) basis for all fields. The complete set of interaction vertices can be derived including all or any chosen subset of SMEFT operators. As an option, the user can also choose preferred gauge fixing, generating Feynman rules in unitary or $R_\\xi$-gauges (the latter include generation of"},"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":"1904.03204","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-04-05T18:00:32Z","cross_cats_sorted":[],"title_canon_sha256":"c03478a2861ad67aa54cd6887232f3e96f45f0dcb27974a7ca89cd71afc4abed","abstract_canon_sha256":"64dc6f63dea23789f8f6853172ca5154a4391598f26a917244617900a3e07478"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:22:38.385735Z","signature_b64":"TjVLUh9Ndj7KAEGYAcF2aZpt+B3XB1LLNa8UL2Nyjf6Vz8loFpGSCz2duvv6OQqdRTbQt2tOvAEDTbiBPPNSDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"548c3080c68e736aaf02f5c71f044c4955279b73464d90db863905eff87914ac","last_reissued_at":"2026-07-05T00:22:38.385270Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:22:38.385270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SmeftFR -- Feynman rules generator for the Standard Model Effective Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Dedes, J. Rosiek, K. Suxho, L. Trifyllis, M. Paraskevas","submitted_at":"2019-04-05T18:00:32Z","abstract_excerpt":"We present SmeftFR, a Mathematica package designed to generate the Feynman rules for the Standard Model Effective Field Theory (SMEFT) including the complete set of gauge invariant operators up to dimension~6. Feynman rules are generated with the use of FeynRules package, directly in the physical (mass eigenstates) basis for all fields. The complete set of interaction vertices can be derived including all or any chosen subset of SMEFT operators. As an option, the user can also choose preferred gauge fixing, generating Feynman rules in unitary or $R_\\xi$-gauges (the latter include generation of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.03204","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/1904.03204/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":"1904.03204","created_at":"2026-07-05T00:22:38.385324+00:00"},{"alias_kind":"arxiv_version","alias_value":"1904.03204v1","created_at":"2026-07-05T00:22:38.385324+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.03204","created_at":"2026-07-05T00:22:38.385324+00:00"},{"alias_kind":"pith_short_12","alias_value":"KSGDBAGGRZZW","created_at":"2026-07-05T00:22:38.385324+00:00"},{"alias_kind":"pith_short_16","alias_value":"KSGDBAGGRZZWVLYC","created_at":"2026-07-05T00:22:38.385324+00:00"},{"alias_kind":"pith_short_8","alias_value":"KSGDBAGG","created_at":"2026-07-05T00:22:38.385324+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"1906.12310","citing_title":"Proposal for the validation of Monte Carlo implementations of the standard model effective field theory","ref_index":7,"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":18,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22608","citing_title":"Recent Developments in SMEFT: Theory, Tools, and Phenomenology","ref_index":53,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF","json":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF.json","graph_json":"https://pith.science/api/pith-number/KSGDBAGGRZZWVLYC6XDR6BCMJF/graph.json","events_json":"https://pith.science/api/pith-number/KSGDBAGGRZZWVLYC6XDR6BCMJF/events.json","paper":"https://pith.science/paper/KSGDBAGG"},"agent_actions":{"view_html":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF","download_json":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF.json","view_paper":"https://pith.science/paper/KSGDBAGG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1904.03204&json=true","fetch_graph":"https://pith.science/api/pith-number/KSGDBAGGRZZWVLYC6XDR6BCMJF/graph.json","fetch_events":"https://pith.science/api/pith-number/KSGDBAGGRZZWVLYC6XDR6BCMJF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF/action/storage_attestation","attest_author":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF/action/author_attestation","sign_citation":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF/action/citation_signature","submit_replication":"https://pith.science/pith/KSGDBAGGRZZWVLYC6XDR6BCMJF/action/replication_record"}},"created_at":"2026-07-05T00:22:38.385324+00:00","updated_at":"2026-07-05T00:22:38.385324+00:00"}