TY - JOUR
T1 - Search for single production of vector-like quarks decaying into Wb in pp collisions at s√ = 13 TeV with the ATLAS detector
AU - Bethani, Agni
AU - Bitadze, Alexander
AU - Crane, Jonathan
AU - Da Via, Cinzia
AU - Dann, Nicholas
AU - Dysch, Sam
AU - Forti, Alessandra
AU - Hanson, Emily
AU - Howarth, James
AU - Lack, David
AU - Lopez Paz, Ivan
AU - Masik, Jiri
AU - Menary, Stephen
AU - Munoz Sanchez, Francisca
AU - Oh, Alexander
AU - Pater, Joleen
AU - Peters, Yvonne
AU - Pickles, Rebecca
AU - Pilkington, Andrew
AU - Price, Darren
AU - Qin, Yang
AU - Rawling, Jacob
AU - Scharmberg, Nicolas
AU - Shaw, Savanna
AU - Wyatt, Terence
PY - 2019
Y1 - 2019
N2 - A search for singly produced vector-like quarks Q, where Q can be either a T quark with charge +2/3 or a Y quark with charge −4/3, is performed in proton–proton collision data at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the LHC in 2015 and 2016. The analysis targets Q → Wb decays where the W boson decays leptonically. No significant deviation from the expected Standard Model background is observed. Upper limits are set on the QWb coupling strength and the mixing between the Standard Model sector and a singlet T quark or a Y quark from a (B, Y) doublet or a (T, B, Y) triplet, taking into account the interference effects with the Standard Model background. The upper limits set on the mixing angle are as small as |sin θL| = 0.18 for a singlet T quark of mass 800 GeV, |sin θR| = 0.17 for a Y quark of mass 800 GeV in a (B, Y) doublet model and |sin θL| = 0.16 for a Y quark of mass 800 GeV in a (T, B, Y) triplet model. Within a (B, Y) doublet model, the limits set on the mixing parameter |sin θR| are comparable with the exclusion limits from electroweak precision observables in the mass range between about 900 GeV and 1250 GeV.
AB - A search for singly produced vector-like quarks Q, where Q can be either a T quark with charge +2/3 or a Y quark with charge −4/3, is performed in proton–proton collision data at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the LHC in 2015 and 2016. The analysis targets Q → Wb decays where the W boson decays leptonically. No significant deviation from the expected Standard Model background is observed. Upper limits are set on the QWb coupling strength and the mixing between the Standard Model sector and a singlet T quark or a Y quark from a (B, Y) doublet or a (T, B, Y) triplet, taking into account the interference effects with the Standard Model background. The upper limits set on the mixing angle are as small as |sin θL| = 0.18 for a singlet T quark of mass 800 GeV, |sin θR| = 0.17 for a Y quark of mass 800 GeV in a (B, Y) doublet model and |sin θL| = 0.16 for a Y quark of mass 800 GeV in a (T, B, Y) triplet model. Within a (B, Y) doublet model, the limits set on the mixing parameter |sin θR| are comparable with the exclusion limits from electroweak precision observables in the mass range between about 900 GeV and 1250 GeV.
U2 - 10.1007/JHEP05(2019)164
DO - 10.1007/JHEP05(2019)164
M3 - Article
SN - 1126-6708
JO - The Journal of High Energy Physics
JF - The Journal of High Energy Physics
ER -