We study the collider phenomenology of the lightest Kaluza-Klein excitation of the gluon, G*, in theories with a warped extra dimension. We do so by means of a two-site effective lagrangian which includes only the lowest-lying spin-1 and spin-1/2 resonances. We point out the importance of the decays of G* to one SM plus one heavy fermion, that were overlooked in the previous literature. It turns out that, when kinematically allowed, such heavy-light decays are powerful channels for discovering the G*. In particular, we present a parton-level Montecarlo analysis of the final state Wtb that follows from the decay of G* to one SM top or bottom quark plus its heavy partner. We find that at \sqrts = 7 TeV and with 10 fb^-1 of integrated luminosity, the LHC can discover a KK gluon with mass in the range M_G* = (1.8 - 2.2) TeV if its coupling to a pair of light quarks is g_G*qqbar = (0.2-0.5) g_3. The same process is also competitive for the discovery of the top and bottom partners as well. We find, for example, that the LHC at \sqrts = 7 TeV can discover a 1 TeV KK bottom quark with an integrated luminosity of (5.3 - 0.61) fb^-1 for g_G*qqbar = (0.2-0.5)

### Heavy-light decay topologies as a new strategy to discover a heavy gluon

#### Abstract

We study the collider phenomenology of the lightest Kaluza-Klein excitation of the gluon, G*, in theories with a warped extra dimension. We do so by means of a two-site effective lagrangian which includes only the lowest-lying spin-1 and spin-1/2 resonances. We point out the importance of the decays of G* to one SM plus one heavy fermion, that were overlooked in the previous literature. It turns out that, when kinematically allowed, such heavy-light decays are powerful channels for discovering the G*. In particular, we present a parton-level Montecarlo analysis of the final state Wtb that follows from the decay of G* to one SM top or bottom quark plus its heavy partner. We find that at \sqrts = 7 TeV and with 10 fb^-1 of integrated luminosity, the LHC can discover a KK gluon with mass in the range M_G* = (1.8 - 2.2) TeV if its coupling to a pair of light quarks is g_G*qqbar = (0.2-0.5) g_3. The same process is also competitive for the discovery of the top and bottom partners as well. We find, for example, that the LHC at \sqrts = 7 TeV can discover a 1 TeV KK bottom quark with an integrated luminosity of (5.3 - 0.61) fb^-1 for g_G*qqbar = (0.2-0.5)
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Utilizza questo identificativo per citare o creare un link a questo documento: `https://hdl.handle.net/11384/64334`
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