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<oembed><version>1.0</version><provider_name>KMI - Nagoya University</provider_name><provider_url>https://www.kmi.nagoya-u.ac.jp/eng</provider_url><title>Tree-level new physics searches in B decays to tau leptons - KMI - Nagoya University</title><type>rich</type><width>600</width><height>338</height><html>&lt;blockquote class="wp-embedded-content" data-secret="rMnss1dykE"&gt;&lt;a href="https://www.kmi.nagoya-u.ac.jp/eng/seminar/974/"&gt;Tree-level new physics searches in B decays to tau leptons&lt;/a&gt;&lt;/blockquote&gt;&lt;iframe sandbox="allow-scripts" security="restricted" src="https://www.kmi.nagoya-u.ac.jp/eng/seminar/974/embed/#?secret=rMnss1dykE" width="600" height="338" title="&#x201C;Tree-level new physics searches in B decays to tau leptons&#x201D; &#x2014; KMI - Nagoya University" data-secret="rMnss1dykE" frameborder="0" marginwidth="0" marginheight="0" scrolling="no" class="wp-embedded-content"&gt;&lt;/iframe&gt;&lt;script type="text/javascript"&gt;
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</html><description>In the SM, the semileptonic decay B &#x2192; D(*) tau nu proceeds via a tree-level process with an intermediate W boson. The charged Higgs boson in supersymmetry or two-Higgs doublet models might give a significant contribution to this decay due to large mass of tau lepton. Although the branching fractions of these decays are a few percent level, it is not so easy to detect them due to the multiple neutrinos in final state. B &#x2192; D* tau nu decay &hellip;</description></oembed>
