@Article{ATLASCollaborationAad_etal2014,
author="ATLAS Collaboration (Aad, G. et al
and Cabrera Urban, S.
and Castillo Gimenez, V.
and Costa, M. J.
and Ferrer, A.
and Fiorini, L.
and Fuster, J.
and Garcia, C.
and Garcia Navarro, J. E.
and Gonzalez de la Hoz, S.
and Hernandez Jimenez, Y.
and Higon-Rodriguez, E.
and Irles Quiles, A.
and Kaci, M.
and King, M.
and Lacasta, C.
and Lacuesta, V. R.
and March, L.
and Marti-Garcia, S.
and Mitsou, V. A.
and Moles-Valls, R.
and Oliver Garcia, E.
and Pedraza Lopez, S.
and Perez Garcia-Esta{\~A}{\textpm}, M. T.
and Romero Adam, E.
and Ros, E.
and Salt, J.
and Sanchez Martinez, V.
and Soldevila, U.
and Sanchez, J.
and Torro Pastor, E.
and Valero, A.
and Valladolid Gallego, E.
and Valls Ferrer, J. A.
and Vos, M.",
title="Comprehensive measurements of t-channel single top-quark production cross sections at root S=7 TeV with the ATLAS detector",
journal="Physical Review D",
year="2014",
publisher="Amer Physical Soc",
volume="90",
number="11",
pages="112006--45pp",
abstract="This article presents measurements of the t-channel single top-quark ((t) over bart) and top-antiquark ({\textit{} t) total production cross sections sdtq{}} and sd {\textit{} tq{}}, their ratio Rt sdtq{\textit{}= sd {}} tq{\textit{}, and a measurement of the inclusive production cross section sdtq {}} {\textit{} tq{}} in proton-proton collisions at ffiffiffi ps = 7 TeV at the LHC. Differential cross sections for the tq and {\textit{} tq processes are measured as a function of the transverse momentum and the absolute value of the rapidity of t and {}} t, respectively. The analyzed data set was recorded with the ATLAS detector and corresponds to an integrated luminosity of 4.59 fb-1. Selected events contain one charged lepton, large missing transverse momentum, and two or three jets. The cross sections are measured by performing a binned maximum-likelihood fit to the output distributions of neural networks. The resulting measurements are sdtq{\textit{} 46 = 1dstat{}} = 6dsyst{\textit{} pb, sd {}} tq{\textit{} = 23 +/- 1dstat{}} = 3dsyst{\textit{} pb, Rt = 2.04 0.13dstat{}} +/-=0.12dsyst{\textit{}, and sdtq {}} {\textit{} tq{}} = 68 +/-= 2dstat{\textit{} = 8dsyst{}} pb, consistent with the Standard Model expectation. The uncertainty on the measured cross sections is dominated by systematic uncertainties, while the uncertainty on Rt is mainly statistical. Using the ratio of sdtq {\textit{} {}} tq{\_} to its theoretical prediction, and assuming that the top-quark-related CKM matrix elements obey the relation jVtbj = jVtsj; jVtdj, we determine jVtbj = 1.02 = 0.07.",
optnote="WOS:000346377100003",
optnote="exported from refbase (https://references.ific.uv.es/refbase/show.php?record=2047), last updated on Thu, 15 Jan 2015 11:47:05 +0000",
issn="1550-7998",
doi="10.1103/PhysRevD.90.112006",
opturl="http://arxiv.org/abs/1406.7844",
opturl="https://doi.org/10.1103/PhysRevD.90.112006",
archivePrefix="arXiv",
eprint="1406.7844",
language="English"
}