München, Univ., Diss., 2001. / Computerdatei im Fernzugriff.

München, Univ., Diss., 2001. / Computerdatei im Fernzugriff.

Wuppertal, Universiẗat, Diss., 2000.

A measurement of the W+ and W− cross section in the electron channel is presented. The measurement is performed using data collected with the ATLAS experiment in 2011, amounting to an integrated luminosity of 4.58 fb⁻¹. The centre of mass energy is √s = 7 TeV. The measurement is performed differentially in the electron pseudorapidity. The W charge asymmetry is also presented. The results are compared to theoretical predictions calculated at next-to-next-to-leading order in perturbative QCD using various Parton Distribution Functions.

Berlin, Humboldt-University, Diss., 2001.

A first measurement of Electroweak W + 2 jets production at high dijet mass is performed using sqrt(s) = 7 TeV pp collision data from the Atlas experiment corresponding to 4.6 fb−1 of integrated luminosity. The background only hypothesis is excluded with a significance of 4.89-σ. A cross section of σ = 325 ± 6 (lumi) ±32 (stat) +63−70(syst) ±86 (theo) fb is extracted in the fiducial region.

The first measurement of the production cross section for a single top quark in association with a W boson with the CMS experiment at the Large Hadron Collider is presented. The analysed data is from proton-proton collisions at a centre-of-mass energy of 7 TeV, corresponding to an integrated luminosity of 4.9 fb-1. The analysis focuses on the leptonic final states of the process and implements a cut-based method. The final state consists of two leptons, two neutrinos and a jet from the fragmentation of a b-quark. The primary source of background events arises from tt(overbar) production, followed by Z/gamma* processes. The observed signal has a significance of 3:5sigma and corresponds to a cross section measurement of 14:9+5:0 -5:1 (stat + syst) pb, in agreement with the Standard Model expectations.

In this thesis we examine the vector boson scattering (VBS) process \(\mathrm p \mathrm p \to \mathrm e^+ \nu_\mathrm e\mu^-\bar\nu_\mu\mathrm j\mathrm j +X\) (short: \(\mathrm W^+\mathrm W^-\) scattering) at NLO accuracy in two experimental setups by performing a Monte Carlo analysis of a \(13\,\mathrm{TeV}\) LHC run. \(\mathrm W^+\mathrm W^-\) scattering shows similarities and differences compared to the scattering of other vector bosons. We present a detailed description of the types of appearing subprocesses and background processes. We give insight into our code which solves the problems we are faced within \(\mathrm W^+\mathrm W^-\) scattering. This is especially the presence of the Higgs-boson resonance in the fiducial phase-space region. Particular attention is dedicated to the permutation of resonances. The integrated signal cross section at LO \(\mathcal O(\alpha^6)\) amounts to \(2.6988(3)\,\mathrm{fb}\) and \(1.5322(2)\,\mathrm{fb}\), respectively, in the two experimental setups. The LO QCD-induced background of \(\mathcal O(\alpha_\mathrm s^2\alpha^4)\) amounts to \(6.9115(9)\,\mathrm{fb}\) and \(1.6923(3)\,\mathrm{fb}\). The EW corrections to the signal are \(-11.4\%\) and \(-6.7\%\), the QCD corrections amount to \(-5.2\%\) and \(-23.0\%\). The EW corrections to the background are \(-8.3\%\) and \(-5.3\%\), the QCD corrections amount to \(-30.3\%\) and \(-77.6\%\). Our results for the QCD corrections and the QCD-induced background include a large uncertainty from varying the renormalisation and factorisation scale, and we discuss improvements for future calculations. We show the differential cross sections with unique features of \(\mathrm W^+\mathrm W^-\) scattering compared to other VBS processes and investigate in particular the subprocess of Higgs-boson production by using a modified version of our setups. / In dieser Arbeit untersuchen wir den Vektorboson-Streuprozess (VBS-Prozess) \(\mathrm p\mathrm p \to \mathrm e^+\nu_\mathrm e\mu^-\bar\nu_\mu\mathrm j\mathrm j + X\) (kurz: \(\mathrm W^+\mathrm W^-\)-Streuung) auf nächstführender Ordnung in zwei Versuchsanordnungen, indem wir eine Monte-Carlo-Analyse des LHC-Betriebs bei \(13\,\mathrm{TeV}\) durchführen. \(\mathrm W^+\mathrm W^-\)-Streuung zeigt Gemeinsamkeiten mit der und Unterschiede zur Streuung anderer Vektorbosonen. Wir stellen eine detaillierte Beschreibung der Arten auftauchender Subprozesse und Hintergrundprozesse vor und geben Einsicht in unseren Code, der die Probleme löst, vor die wir im Rahmen der \(\mathrm W^+\mathrm W^-\)-Streuung gestellt wurden. Dies ist insbesondere die Präsenz der Higgs-Boson-Resonanz im Bezugsphasenraum. Besonderes Augenmerk wird auf die Permutation der Resonanzen gelegt. Wir präsentieren den integrierten Wirkungsquerschnitt. Der integrierte Wirkungsquerschnitt des Signals beträgt \(2{,}6988(3)\,\mathrm{fb}\) beziehungsweise \(1{,}5322(2)\,\mathrm{fb}\) auf führender Ordnung \(\mathcal O(\alpha^6)\) in den beiden experimentellen Setups. Der QCD-Hintergrund auf führender Ordnung \(\mathcal O(\alpha_\mathrm s^2\alpha^4)\) beträgt \(6{,}9115(9)\,\mathrm{fb}\) bzw. \(1{,}6923(3)\,\mathrm{fb}\). Die elektroschwachen Korrekturen zum Signal belaufen sich auf \(-11{,}4\%\) bzw. \(-6{,}7\%\), die QCD-Korrekturen auf \(-5{,}2\%\) bzw. \(-23{,}0\%\). Die elektroschwachen Korrekturen zum Hintergrund sind \(-8{,}3\%\) bzw. \(-5{,}3\%\), die QCD-Korrekturen \(-30{,}3\%\) bzw. \(-77{,}6\%\). Unsere Ergebnisse für die QCD-Korrekturen und den QCD-induzierten Hintergrund enthalten eine große Unsicherheit durch die Variation der Renormierungs- und Faktorisierungsskala und wir diskutieren Verbesserungen für zukünftige Rechnungen. Wir zeigen die differentiellen Wirkungsquerschnitte mit Eigenheiten von \(\mathrm W^+\mathrm W^-\)-Streuung verglichen mit anderen VBS-Prozessen und betrachten insbesondere den Subprozess der Higgs-Boson-Produktion, indem wir eine modifizierte Version unserer Versuchsanordnungen verwenden.

This thesis presents the measurement of the production cross section of a W boson with a single charm quark in 7 TeV proton-proton collisions using the ATLAS detector at the Large Hadron Collider. The data analysed correspond to an integrated luminosity of 4.6 fb 1 and were collected during 2011. This is the first time that ATLAS data has been used for this particular measurement. This cross section is of particular interest as a probe of the strange quark density of the proton. Typically, the strange quark density is considered to be suppressed relative to that of the other light-quarks in the proton sea. However, some analyses suggest a more symmetric composition of light-quarks in the proton sea. The results of this study aim to improve the precision of the determination of the strange quark density. The analysis uses events where the W boson decays to a muon and a neutrino. In such events, the charm quark is identified by its semileptonic decay to a soft muon within a hadronic jet. The charge correlation between the W boson and the soft muon is exploited to reduce the backgrounds substantially. The analysis results are combined with those obtained using additional decay channels. The measured cross section provides further constraint for the determination of the strange quark density, advancing the knowledge of the fundamental structure of the proton. The results are compared with predictions of next-to-leading-order QCD calculations obtained using various parton distribution function parameterisations. Additionally, the ratio of the strange-to-down sea-quark distributions is determined to be 0.96+0.26 0.30 at Q2 = 1.9 GeV2. This supports the hypothesis of a symmetric composition of light-quarks in the proton sea. The cross section ratio (W+ + c)= (W + c) is also determined and compared with different predictions for the asymmetry of the strange and anti-strange quark distribution functions.

This thesis presents studies of the single top t-channel in the electron plus jets mode. In order to understand this channel, an account of the present theoretical models is given. This work relies on collisions data from the ATLAS detector and its components are presented here. A summary of the work involving the SCT, part of the tracking system in ATLAS, is also explained here. Studies were performed to optimize the measurement of the Lorentz Angle of the holes in the Silicon for the initial data taking period. The data studied was acquired by ATLAS during 2011, with a total integrated luminosity of 4.7 pb−1 at a √s = 7 TeV. Monte Carlo simulation of signal and background events was also used throughout. Background studies were performed to correctly determine the expected amount of QCD via the Jet Electron data-driven method and of light or heavy flavour jets produced in association with a W boson, which is one of the dominant backgrounds for the t-channel. A cut based analysis was then applied to the data and simulation in order to better discriminate the t-channel signal. A binned likelihood fit to the invariant mass of the reconstructed top quark was performed and the cross section value for the t-channel process was calculated: σt−channel = 62.2±8.0(stat)+8.6 −8.8(syst) pb which is in good agreement with the theoretically predicted value. Finally, the response (preco T /ptrue T ) of light quark or gluon initiated jets is evaluated for both the t-channel and the Wt associated production, in order to determine the flavour composition uncertainty, as part of the framework that provides the jet energy scale uncertainties in a multiple jets environment. Other sources of system- atics are also reviewed.