{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:WXQFHQ324FLVYHSYI266DVJPFF","short_pith_number":"pith:WXQFHQ32","schema_version":"1.0","canonical_sha256":"b5e053c37ae1575c1e5846bde1d52f296fd1a4eb595effa44164dc14afc94133","source":{"kind":"arxiv","id":"2310.11055","version":2},"attestation_state":"computed","paper":{"title":"Revisiting Renormalization Group Equations of the SMEFT Dimension-Seven Operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Di Zhang","submitted_at":"2023-10-17T07:48:24Z","abstract_excerpt":"In this work, we revisit the renormalization group equations (RGEs) of dimension-seven (dim-7) operators in the Standard Model effective field theory (SMEFT) resulting from mixing among dim-7 operators themselves by means of the background field method. Adopting a recently proposed physical basis for dim-7 operators, we achieve the explicit RGEs of all non-redundant dim-7 operators in the SMEFT for the first time. Together with those originating from the dim-5 and dim-6 operators, these results constitute the complete RGEs of dim-7 operators, and hence can be exploited to study full RG-running"},"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":"2310.11055","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-10-17T07:48:24Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"fbe32e65a90bc85378f8e5d443892b9fbf42481ef1341ec3a549ded0bf251cd0","abstract_canon_sha256":"48ec75c53010b8ced31512843a634712e63444739a92c124b15d3d339ce8f936"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:40:02.884565Z","signature_b64":"uWl+wcpAniNWUPVrZdCzVnNf3TFwl0LaCdO3ECC/SUN8uQ7cMD+Erwn7Jd9hD+IY8BE/cbVagBLwOLnbQ4vyCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b5e053c37ae1575c1e5846bde1d52f296fd1a4eb595effa44164dc14afc94133","last_reissued_at":"2026-07-05T07:40:02.884092Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:40:02.884092Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting Renormalization Group Equations of the SMEFT Dimension-Seven Operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Di Zhang","submitted_at":"2023-10-17T07:48:24Z","abstract_excerpt":"In this work, we revisit the renormalization group equations (RGEs) of dimension-seven (dim-7) operators in the Standard Model effective field theory (SMEFT) resulting from mixing among dim-7 operators themselves by means of the background field method. Adopting a recently proposed physical basis for dim-7 operators, we achieve the explicit RGEs of all non-redundant dim-7 operators in the SMEFT for the first time. Together with those originating from the dim-5 and dim-6 operators, these results constitute the complete RGEs of dim-7 operators, and hence can be exploited to study full RG-running"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.11055","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2310.11055/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":"2310.11055","created_at":"2026-07-05T07:40:02.884149+00:00"},{"alias_kind":"arxiv_version","alias_value":"2310.11055v2","created_at":"2026-07-05T07:40:02.884149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.11055","created_at":"2026-07-05T07:40:02.884149+00:00"},{"alias_kind":"pith_short_12","alias_value":"WXQFHQ324FLV","created_at":"2026-07-05T07:40:02.884149+00:00"},{"alias_kind":"pith_short_16","alias_value":"WXQFHQ324FLVYHSY","created_at":"2026-07-05T07:40:02.884149+00:00"},{"alias_kind":"pith_short_8","alias_value":"WXQFHQ32","created_at":"2026-07-05T07:40:02.884149+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26097","citing_title":"Positron-Emitting and Electron-Capturing Double-Beta Processes in the Standard Model and Beyond","ref_index":66,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF","json":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF.json","graph_json":"https://pith.science/api/pith-number/WXQFHQ324FLVYHSYI266DVJPFF/graph.json","events_json":"https://pith.science/api/pith-number/WXQFHQ324FLVYHSYI266DVJPFF/events.json","paper":"https://pith.science/paper/WXQFHQ32"},"agent_actions":{"view_html":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF","download_json":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF.json","view_paper":"https://pith.science/paper/WXQFHQ32","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2310.11055&json=true","fetch_graph":"https://pith.science/api/pith-number/WXQFHQ324FLVYHSYI266DVJPFF/graph.json","fetch_events":"https://pith.science/api/pith-number/WXQFHQ324FLVYHSYI266DVJPFF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF/action/storage_attestation","attest_author":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF/action/author_attestation","sign_citation":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF/action/citation_signature","submit_replication":"https://pith.science/pith/WXQFHQ324FLVYHSYI266DVJPFF/action/replication_record"}},"created_at":"2026-07-05T07:40:02.884149+00:00","updated_at":"2026-07-05T07:40:02.884149+00:00"}