{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JSTBZVY2SXYLDT5N6HAWGI2FQR","short_pith_number":"pith:JSTBZVY2","schema_version":"1.0","canonical_sha256":"4ca61cd71a95f0b1cfadf1c1632345846166758c5f8fe4a5b06da7724c8a1270","source":{"kind":"arxiv","id":"2405.20371","version":1},"attestation_state":"computed","paper":{"title":"A log story short: running contributions to radiative Higgs decays in the SMEFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christophe Grojean, Gabriel M. Salla, Guilherme Guedes, Jasper Roosmale Nepveu","submitted_at":"2024-05-30T18:00:00Z","abstract_excerpt":"We investigate the renormalization of the radiative decays of the Higgs to two gauge bosons in the Standard Model Effective Field Theory at mass dimension eight. Given that these are loop-level processes, their one-loop renormalization can be phenomenologically important when triggered by operators generated through the tree-level exchange of heavy particles (assuming a weakly coupled UV model). By computing the tree-level matching conditions of all relevant extensions of the Standard Model, we demonstrate that this effect is indeed present in the $h\\to \\gamma Z$ decay at dimension eight, even"},"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":"2405.20371","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-30T18:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"afcb67398cbed506b3426d679a74532551d68ce35bf400e30ac16a6001edea39","abstract_canon_sha256":"b75a20be0b7112465a8ca27bab57d310aff84a34e9f314f8933e793cb64e505d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:25:36.575250Z","signature_b64":"aon3rCKZqP6hAhzy9CZD5A+puYVHzLZmKEYZSA2oTk7VUOxD51xhKz9bIqJjt8Ffoikzrf4ZwVfn+iPo2tDuAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ca61cd71a95f0b1cfadf1c1632345846166758c5f8fe4a5b06da7724c8a1270","last_reissued_at":"2026-07-05T08:25:36.574618Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:25:36.574618Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A log story short: running contributions to radiative Higgs decays in the SMEFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christophe Grojean, Gabriel M. Salla, Guilherme Guedes, Jasper Roosmale Nepveu","submitted_at":"2024-05-30T18:00:00Z","abstract_excerpt":"We investigate the renormalization of the radiative decays of the Higgs to two gauge bosons in the Standard Model Effective Field Theory at mass dimension eight. Given that these are loop-level processes, their one-loop renormalization can be phenomenologically important when triggered by operators generated through the tree-level exchange of heavy particles (assuming a weakly coupled UV model). By computing the tree-level matching conditions of all relevant extensions of the Standard Model, we demonstrate that this effect is indeed present in the $h\\to \\gamma Z$ decay at dimension eight, even"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.20371","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/2405.20371/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":"2405.20371","created_at":"2026-07-05T08:25:36.574703+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.20371v1","created_at":"2026-07-05T08:25:36.574703+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.20371","created_at":"2026-07-05T08:25:36.574703+00:00"},{"alias_kind":"pith_short_12","alias_value":"JSTBZVY2SXYL","created_at":"2026-07-05T08:25:36.574703+00:00"},{"alias_kind":"pith_short_16","alias_value":"JSTBZVY2SXYLDT5N","created_at":"2026-07-05T08:25:36.574703+00:00"},{"alias_kind":"pith_short_8","alias_value":"JSTBZVY2","created_at":"2026-07-05T08:25:36.574703+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2412.18540","citing_title":"Higgs Decays to $Z\\gamma$ and $\\gamma\\gamma$ in the Flavor-Gauged Two Higgs Doublet Model","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2412.14253","citing_title":"From the EFT to the UV: the complete SMEFT one-loop dictionary","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR","json":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR.json","graph_json":"https://pith.science/api/pith-number/JSTBZVY2SXYLDT5N6HAWGI2FQR/graph.json","events_json":"https://pith.science/api/pith-number/JSTBZVY2SXYLDT5N6HAWGI2FQR/events.json","paper":"https://pith.science/paper/JSTBZVY2"},"agent_actions":{"view_html":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR","download_json":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR.json","view_paper":"https://pith.science/paper/JSTBZVY2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.20371&json=true","fetch_graph":"https://pith.science/api/pith-number/JSTBZVY2SXYLDT5N6HAWGI2FQR/graph.json","fetch_events":"https://pith.science/api/pith-number/JSTBZVY2SXYLDT5N6HAWGI2FQR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR/action/storage_attestation","attest_author":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR/action/author_attestation","sign_citation":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR/action/citation_signature","submit_replication":"https://pith.science/pith/JSTBZVY2SXYLDT5N6HAWGI2FQR/action/replication_record"}},"created_at":"2026-07-05T08:25:36.574703+00:00","updated_at":"2026-07-05T08:25:36.574703+00:00"}