2014
DOI: 10.1007/jhep10(2014)188
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RS resonance in di-final state production at the LHC to NLO+PS accuracy

Abstract: We study the di-final state processes ($\ell^+ \ell^-$, $\gamma \gamma$, $ZZ$, $W^+ W^-$) to NLO+PS accuracy, as a result of both the SM and RS Kaluza-Klein graviton excitations. Decay of the electroweak gauge boson final states to different leptonic states are included at the showering stage. A selection of the results has been presented with PDF and scale uncertainties for various distributions. Using the di-lepton and di-photon final states, we present the search sensitivity, for the $14$ TeV LHC at $50$ fb… Show more

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Cited by 19 publications
(24 citation statements)
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“…These include simplified models, in which the SM is extended by colour-triplet and octet scalar particles [73,169], both gluinos and squarks [74] or sleptons [90], as well as by vectorlike quarks [170,171], a heavy top-philic scalar [172] or a spin-2 particle [173]. In the latter spin-2 case, new physics have also been previously explored in a semi-automated framework (in the sense where the virtual matrix elements are provided externally) based on MG5 aMC [174][175][176]. Various BSM setups in which the Higgs sector differs from the SM one have been released, such as the two-Higgs-doublet model [177,178], the Georgi-Machacek model [179], the Higgs characterisation model [180][181][182][183][184], and the SM effective field theory including dimension-six operators [185].…”
Section: Simulations and Cross Section Calculations In Susymentioning
confidence: 99%
“…These include simplified models, in which the SM is extended by colour-triplet and octet scalar particles [73,169], both gluinos and squarks [74] or sleptons [90], as well as by vectorlike quarks [170,171], a heavy top-philic scalar [172] or a spin-2 particle [173]. In the latter spin-2 case, new physics have also been previously explored in a semi-automated framework (in the sense where the virtual matrix elements are provided externally) based on MG5 aMC [174][175][176]. Various BSM setups in which the Higgs sector differs from the SM one have been released, such as the two-Higgs-doublet model [177,178], the Georgi-Machacek model [179], the Higgs characterisation model [180][181][182][183][184], and the SM effective field theory including dimension-six operators [185].…”
Section: Simulations and Cross Section Calculations In Susymentioning
confidence: 99%
“…Often, these observables suffer from large uncertainties resulting from renormalization and factorization scales and the only remedy to this is to include higher order QCD effects to the Born contributions. The NLO QCD predictions based on fixed order as well as parton shower improved in the MadGraph5 aMC@NLO [33] framework for di-final state [34][35][36][37][38][39][40][41][42] productions in the gravity mediated models have already played important role in constraining the parameters of ADD and RS models. Next-to-next-to leading order (NNLO) corrections for the graviton production at the LHC in the threshold limit are already available [43] and attempts to improve these predictions through NNLO corrections and beyond are already underway [44].…”
Section: Jhep12(2015)084mentioning
confidence: 99%
“…NLO QCD corrections have been computed for the extra dimension models viz. ADD and RS for most of the di-final state process [28][29][30][31][32][33][34][35] and this has been extended to NLO+PS accuracy [36][37][38]. Recently, for the di-lepton production to NNLO order in QCD for the ADD model was computed [39].…”
Section: Introductionmentioning
confidence: 99%