Top quark pair production (tt¯) can be studied at the LHC with unprecented statis tics. In this thesis, studies performed at the ATLAS experiment exploiting the dilepton channel, i.e. events where both top quarks decaying to t → W b have a subsequent W± → ` ±ν (` ± = e ±, µ±) decay, are presented. A search for a Be yond Standard Model (BSM) resonance is perfomed considering the full pp collision dataset collected by ATLAS at √ s = 13 TeV, using two different invariant mass variables (m``bb and mNW tt¯ ), each combined with a spin-sensitive variable (∆φ ``). Expected mass limits for three different BSM models, at 95% confidence level, are obtained. A neutral heavy gauge boson Z 0 with a mass smaller than 2.4 TeV (2.0 TeV) can be excluded if using m``bb (mNW tt¯ ). A Randall-Sundrum graviton G, with a mass smaller than 1 TeV (0.9 TeV) can be excluded if using m``bb (mNW tt¯ ). A Kaluza Klein gluon gKK, with a mass smaller than 3.5 TeV (3.3 TeV) can be excluded if using m``bb (mNW tt¯ ).
DE SANTIS, M. (2020). Search for a beyond the standard model resonance decaying to top quark pair in the dilepton final state with the ATLAS experiment [10.58015/de-santis-maurizio_phd2020].
Search for a beyond the standard model resonance decaying to top quark pair in the dilepton final state with the ATLAS experiment
DE SANTIS, MAURIZIO
2020-01-01
Abstract
Top quark pair production (tt¯) can be studied at the LHC with unprecented statis tics. In this thesis, studies performed at the ATLAS experiment exploiting the dilepton channel, i.e. events where both top quarks decaying to t → W b have a subsequent W± → ` ±ν (` ± = e ±, µ±) decay, are presented. A search for a Be yond Standard Model (BSM) resonance is perfomed considering the full pp collision dataset collected by ATLAS at √ s = 13 TeV, using two different invariant mass variables (m``bb and mNW tt¯ ), each combined with a spin-sensitive variable (∆φ ``). Expected mass limits for three different BSM models, at 95% confidence level, are obtained. A neutral heavy gauge boson Z 0 with a mass smaller than 2.4 TeV (2.0 TeV) can be excluded if using m``bb (mNW tt¯ ). A Randall-Sundrum graviton G, with a mass smaller than 1 TeV (0.9 TeV) can be excluded if using m``bb (mNW tt¯ ). A Kaluza Klein gluon gKK, with a mass smaller than 3.5 TeV (3.3 TeV) can be excluded if using m``bb (mNW tt¯ ).| File | Dimensione | Formato | |
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