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Focusing on the couplings of the muon, the partial decay width of $h\\to e_4^\\pm \\mu^\\mp$, where $e_4$ is the new lepton, can be significant when this process is kinematically allowed. Subsequent decays $e_4^\\pm \\to Z\\mu^\\pm$ and $e_4^\\pm \\to W^\\pm \\nu$ lead to the same final states as $h \\to ZZ^* \\to Z \\mu^+\\mu^-$ and $h \\to WW^* \\to W \\mu\\nu$, thus possibly affecting measurements of these processes. We calculate $h\\to e_4 \\ell_i\n "},"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":"1406.7018","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-06-26T20:09:36Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"441e2e17b2700614dc18eaeab278f14bb44c0b711477a512db4028913ca054c9","abstract_canon_sha256":"cd63e589f48dfac439b2be78c4ea8fadaacbf51e2a39cc96548d725a25e1974b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:34.690341Z","signature_b64":"7GF1jaRIMkWAS7WFOoGOab109xVE2hCEUM8gOGYBGf8ETL//HqUO1NsiKRCOqeYVleWrHuZ2j04lj+mfldPqCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"21fbcb19caf8ea5cef69b68fa07657dfeac789b48c3432ad0d1d86ae50b71040","last_reissued_at":"2026-05-18T02:43:34.689708Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:34.689708Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of vectorlike leptons on $h\\to 4\\ell$ and the connection to the muon g-2 anomaly","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Aditi Raval, Radovan Dermisek, Seodong Shin","submitted_at":"2014-06-26T20:09:36Z","abstract_excerpt":"The mixing of new vectorlike leptons with leptons in the standard model can generate flavor violating couplings of $h$, $W$ and $Z$ between heavy and light leptons. Focusing on the couplings of the muon, the partial decay width of $h\\to e_4^\\pm \\mu^\\mp$, where $e_4$ is the new lepton, can be significant when this process is kinematically allowed. Subsequent decays $e_4^\\pm \\to Z\\mu^\\pm$ and $e_4^\\pm \\to W^\\pm \\nu$ lead to the same final states as $h \\to ZZ^* \\to Z \\mu^+\\mu^-$ and $h \\to WW^* \\to W \\mu\\nu$, thus possibly affecting measurements of these processes. 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