Abstract

This article presents measurements of the $t$-channel single top-quark ($t$) and top-antiquark ($\bar{t}$) total production cross sections $\sigma(tq)$ and $\sigma(\bar{t}q)$, their ratio $R_{t}=\sigma(tq)/\sigma(\bar{t}q)$, and a measurement of the inclusive production cross section $\sigma(tq + \bar{t}q)$ in proton--proton collisions at $\sqrt{s} = 7$ TeV at the LHC. Differential cross sections for the $tq$ and $\bar{t}q$ processes are measured as a function of the transverse momentum and the absolute value of the rapidity of $t$ and $\bar{t}$, 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 $\sigma(tq)= 46\pm 6\; \mathrm{pb}$, $\sigma(\bar{t}q)= 23 \pm 4\; \mathrm{pb}$, $R_{t}=2.04\pm 0.18$, and $\sigma(tq + \bar{t}q)= 68 \pm 8\; \mathrm{pb}$, consistent with the Standard Model expectation. The uncertainty on the measured cross sections is dominated by systematic uncertainties, while the uncertainty on $R_{t}$ is mainly statistical. Using the ratio of $\sigma(tq + \bar{t}q)$ to its theoretical prediction, and assuming that the top-quark-related CKM matrix elements obey the relation $|V_{tb}|\gg |V_{ts}|, |V_{td}|$, we determine $|V_{tb}|=1.02 \pm 0.07$.

Highlights

  • In proton-proton collisions at the LHC, top quarks are produced at unprecedented rates, allowing studies that were intractable before

  • In this article we present measurements of σðtq þtqÞ, σðtqÞ, mass σðtqÞ, energy and of tpheffiffi s cross-section ratio Rt 1⁄4 7 TeV, using the at a full center-ofdata set corresponding to an integrated luminosity of 4.59 fb−1

  • The analysis described in this article uses pp collision data collected at a center-of-mass energy of 7 TeV with the ATLAS detector [20] at the LHC between March and November 2011

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Summary

INTRODUCTION

In proton-proton (pp) collisions at the LHC, top quarks are produced at unprecedented rates, allowing studies that were intractable before. A measurement of the combined top-quark and top-antiquark cross section σðtq þtqÞ 1⁄4 σðtqÞ þ σðtqÞ is well suited to constrain Vtb. 112006-1 or the b-quark PDF. In this article we present measurements of σðtq þtqÞ, σðtqÞ, mass σðtqÞ, energy and of tpheffiffi s cross-section ratio Rt 1⁄4 7 TeV, using the at a full center-ofdata set corresponding to an integrated luminosity of 4.59 fb−1. In pp collisions at s 1⁄4 7 TeV, the total inclusive cross sections of top-quark and top-antiquark production in the t channel are predicted to be σðtqÞ 1⁄4 41.9þ−01..98 pb; σðtqÞ 1⁄4 22.7þ−10..09 pb; and σðtq þtqÞ 1⁄4 64.6þ−22..07 pb; with approximate next-to-next-to-leading-order (NNLO) precision [9], assuming a top-quark mass of mt 1⁄4 172.5 GeV and using the MSTW2008 NNLO [10] PDF set.

DATA SAMPLES AND SAMPLES OF SIMULATED EVENTS
The ATLAS detector
Trigger requirements
Simulated events
PHYSICS OBJECT DEFINITIONS
Electrons
Jets and missing transverse momentum
Identification of b-quark jets
EVENT SELECTION
BACKGROUND
Multijet background
Event yields
SIGNAL AND BACKGROUND DISCRIMINATION
Top-quark reconstruction
Selection of discriminating variables
Neural network training
Extraction of the signal yield
High-purity region
SYSTEMATIC UNCERTAINTIES
Physics object modeling
AAD et al 10000 ATLAS
AAD et al 1500
Monte Carlo generators
Parton distribution function
Theoretical cross-section normalization
Luminosity
Uncertainties on the cross-section measurements
VIII. TOTAL CROSS-SECTION MEASUREMENTS
Cross-section dependence on the top-quark mass
15 Æ 10 59 Æ 30
DIFFERENTIAL CROSS-SECTION MEASUREMENTS
Method
Treatment of uncertainties
Results
ATLAS 10-1 10-2 10-3
Background normalization JES η intercalibration
Findings
CONCLUSIONS
Full Text
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