Abstract

In extensions of the standard model with compactified extra dimensions, perturbative unitarity of the longitudinal gauge bosons is maintained through the contribution of heavy Kaluza-Klein excitations of the gauge fields, without the necessity of introducing a Higgs field. The three-site Higgsless model represents a minimal approach in this respect, containing just one extra set of heavy gauge bosons ${Z}^{\ensuremath{'}}/{W}^{\ensuremath{'}\ifmmode\pm\else\textpm\fi{}}$ in the spectrum. While the ${Z}^{\ensuremath{'}}$ can have robust couplings to SM fermions and, hence, may be detected within the first $1--20\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ of LHC data ($\sqrt{s}=14\text{ }\text{ }\mathrm{TeV}$), the coupling of the ${W}^{\ensuremath{'}}$ to light fermions is suppressed and depends on the model parameters. Expanding on previous parton-level studies, we determine discovery thresholds of the ${W}^{\ensuremath{'}}$ in $s$-channel Drell-Yan production at the LHC for masses ${m}_{{W}^{\ensuremath{'}}}=380$, 500, and 600 GeV, combining analyses of the semileptonic final states $\ensuremath{\ell}\ensuremath{\ell}jj$, $\ensuremath{\ell}\ensuremath{\nu}jj$ and the leptonic final state $\ensuremath{\ell}\ensuremath{\nu}\ensuremath{\ell}\ensuremath{\ell}$ ($\ensuremath{\ell}=e,\ensuremath{\mu}$) including fast detector simulation.

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