{"paper":{"title":"Higgs decays to $\\gamma$ and invisible particles in the standard model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dao-Neng Gao, Yi Sun","submitted_at":"2013-10-31T06:56:33Z","abstract_excerpt":"Using the Higgs boson mass $m_h=125$ GeV, the radiative Higgs decays $h\\rightarrow\\gamma \\nu_l\\bar\\nu_l$ with $\\nu_l = \\nu_e,\\,\\nu_\\mu$ and $\\nu_\\tau$ are analyzed in the standard model. Our calculation shows that the inclusive width of these processes, i.e., the sum of $\\Gamma(h\\to\\gamma\\nu_l\\bar\\nu_l)$ for ${\\nu_l=\\nu_e,\\nu_\\mu,\\nu_\\tau}$, is $1.41$ keV, which is about $15\\%$ of $\\Gamma(h\\to\\gamma\\gamma)$. Therefore, the observation of these channels in the future precise experiments may provide us some useful information on the Higgs physics both in the standard model and in its possible ex"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.8404","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":""},"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"}