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Search for doubly-charged Higgs bosons in same-charge electron pair final states using proton-proton collisions at $\sqrt{s}=13\,\mathrm{TeV}$ with the ATLAS detector

A search for doubly-charged Higgs bosons decaying to pairs of same-charge, isolated, high-pT electrons is presented. Same-charge electron pairs are selected in an inclusive way and the same-charge electron pair invariant mass spectrum is studied. The search uses the $pp$ collision data sample corres...

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Detalles Bibliográficos
Autor principal: The ATLAS collaboration
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:http://cds.cern.ch/record/2206133
Descripción
Sumario:A search for doubly-charged Higgs bosons decaying to pairs of same-charge, isolated, high-pT electrons is presented. Same-charge electron pairs are selected in an inclusive way and the same-charge electron pair invariant mass spectrum is studied. The search uses the $pp$ collision data sample corresponding to $13.9\,\mathrm{fb}^{-1}$ of integrated luminosity collected in 2015 and 2016 by the ATLAS detector at the LHC at the centre-of-mass energy of $13\,\mathrm{TeV}$. A model independent search for new physics processes was performed and no clear evidence for an excess was observed. Therefore, the upper limits for the signal cross-sections were set at 95% confidence level. Consequently, the observed lower mass limits, assuming a $100\%$ branching ratio to electrons ($\mathrm{Br}(H^{\pm \pm}\rightarrow e^{\pm}e^{\pm})=100\%$), are $420\,\mathrm{GeV}$ for a doubly-charged Higgs boson coupling to right-handed leptons ($H_R^{\pm \pm}$) and $570\,\mathrm{GeV}$ for a doubly-charged Higgs boson coupling to left-handed leptons ($H_L^{\pm \pm}$). The expected lower mass limits were $460\,\mathrm{GeV}$ for $H_R^{\pm \pm}$ and $580\,\mathrm{GeV}$ for $H_L^{\pm \pm}$. Limits were also derived with the assumption that $\mathrm{Br}(H^{\pm \pm}\rightarrow e^{\pm}e^{\pm})=50\%$. In this case, the lower mass limits are $380\,\mathrm{GeV}$ for $H_R^{\pm \pm}$ and $530\,\mathrm{GeV}$ for $H_L^{\pm \pm}$. The expected limits for this assumption were $400\,\mathrm{GeV}$ for $H_R^{\pm \pm}$ and $530\,\mathrm{GeV}$ for $H_L^{\pm \pm}$.