TY - JOUR
T1 - Measurement of the inclusive cross-sections of single top-quark and top-antiquark t-channel production in pp collisions at √s=13 TeV with the ATLAS detector
AU - Barnes, Sarah
AU - Bielski, Rafal
AU - Cox, Brian
AU - Da Via, Cinzia
AU - Dann, Nick
AU - Forcolin, Giulio
AU - Forti, Alessandra
AU - Iturbe Ponce, Julia
AU - Li, Xingguo
AU - Loebinger, Frederick
AU - Marsden, Stephen
AU - Masik, Jiri
AU - Munoz Sanchez, Francisca
AU - Neep, Thomas
AU - Oh, Alexander
AU - Ospanov, Rustem
AU - Pater, Joleen
AU - Peters, Yvonne
AU - Pilkington, Andrew
AU - Pin, Arnaud
AU - Price, Darren
AU - Qin, Yang
AU - Raine, John
AU - Shaw, Savanna
AU - Tomlinson, Lee
AU - Watts, Stephen
AU - Wilk, Fabian
AU - Woudstra, Martin
AU - Wyatt, Terence
AU - ATLAS Collaboration
PY - 2017/4/14
Y1 - 2017/4/14
N2 - A measurement of the t-channel single-top-quark and single-top-antiquark production cross-sections in the lepton+jets channel is presented, using 3.2 fb−1 of proton-proton collision data at a centre-of-mass energy of 13 TeV, recorded with the ATLAS detector at the LHC in 2015. Events are selected by requiring one charged lepton (electron or muon), missing transverse momentum, and two jets with high transverse momentum, exactly one of which is required to be b-tagged. Using a binned maximum-likelihood fit to the discriminant distribution of a neural network, the cross-sections are determined to be σ(tq) = 156 ± 5 (stat.) ± 27 (syst.) ± 3 (lumi.) pb for single top-quark production and σ(t¯q)=91±4 (stat.) ± 18 (syst.) ± 2 (lumi.) pb for single top-antiquark production, assuming a top-quark mass of 172.5 GeV. The cross-section ratio is measured to be Rt=σ(tq)/σ(t¯q)=1.72±0.09 (stat.) ± 0.18 (syst.). All results are in agreement with Standard Model predictions.
AB - A measurement of the t-channel single-top-quark and single-top-antiquark production cross-sections in the lepton+jets channel is presented, using 3.2 fb−1 of proton-proton collision data at a centre-of-mass energy of 13 TeV, recorded with the ATLAS detector at the LHC in 2015. Events are selected by requiring one charged lepton (electron or muon), missing transverse momentum, and two jets with high transverse momentum, exactly one of which is required to be b-tagged. Using a binned maximum-likelihood fit to the discriminant distribution of a neural network, the cross-sections are determined to be σ(tq) = 156 ± 5 (stat.) ± 27 (syst.) ± 3 (lumi.) pb for single top-quark production and σ(t¯q)=91±4 (stat.) ± 18 (syst.) ± 2 (lumi.) pb for single top-antiquark production, assuming a top-quark mass of 172.5 GeV. The cross-section ratio is measured to be Rt=σ(tq)/σ(t¯q)=1.72±0.09 (stat.) ± 0.18 (syst.). All results are in agreement with Standard Model predictions.
U2 - 10.1007/JHEP04(2017)086
DO - 10.1007/JHEP04(2017)086
M3 - Article
SN - 1126-6708
VL - 2017
JO - The Journal of High Energy Physics
JF - The Journal of High Energy Physics
IS - 4
M1 - 86
ER -