@phdthesis{Pasold2016, author = {Pasold, Christian}, title = {QCD and electroweak NLO corrections to W + Photon and Z + Photon production including leptonic decays}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-137456}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2016}, abstract = {At a hadron collider as the LHC or the Tevatron the production of a photon in association with a leptonically decaying vector boson represents an important class of processes. These processes stand out due to a very clean signal of a photon and two leptons. Furthermore they provide direct access to the photon-vector-boson couplings and thus an easy opportunity to test the gauge sector of the Standard Model. Within the scope of this work we present a full calculation of the next-to-leading-order corrections which include the O (αs) corrections of the strong interaction as well as the electroweak corrections of O (α) including all photon-induced contributions. For the creation of matrix elements we use methods based on Feynman diagrams. The IR singularities are treated with the dipole subtraction technique. In order to separate photons from jets, a quark-to-photon fragmentation function ´a la Glover / Morgan or Frixione's cone isolation is employed. Moreover, two different scenarios for charged leptons in the fi state were considered. The fi scenario for dressed leptons assumes that a charged lepton and a photon will be recombined if they are collinear. In the second scenario for bare muons it is assumed that leptons and photon can be separated in a detector also if they are collinear. For our calculation we implemented all corrections into a fl Monte Carlo program. Be- sides the computation of the total cross section this program is also able to generate diff tial distributions of several experimentally motivated observables. Apart from the expected large electroweak corrections in the high transverse-momentum regions and sizeable corrections in the resonance regions of the transverse or the invariant masses we found photon-induced corrections up to several 10\% for high transverse momenta. Within run I at the LHC for 7/8 TeV the experimental accuracy for Vγ production was roughly 10\%. Due to the higher luminosity at run II this accuracy will be reduced to the level of a few percent so that corrections of the same order within the theoretical predictions might become relevant. In this work we present results for the total cross section at the LHC for 7, 8 and 14 TeV and the corresponding distributions for 14 TeV.}, subject = {Quantenchromodynamik}, language = {en} } @phdthesis{Lang2017, author = {Lang, Jean-Nicolas Olivier}, title = {Automation of electroweak NLO corrections in general models}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-154426}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2017}, abstract = {The thesis deals with the automated generation and efficient evaluation of scattering amplitudes in general relativistic quantum field theories at one-loop order in perturbation theory. At the present time we lack signals beyond the Standard Model which, in the past, have guided the high-energy physics community, and ultimately led to the discovery of new physics phenomena. In the future, precision tests could acquire this guiding role by systematically probing the Standard Model and constraining Beyond the Standard Model theories. As current experimental constraints strongly favour Standard Model-like theories, only small deviations with respect to the Standard Model are expected which need to be studied in detail. The required precision demands one-loop corrections in all future analyses, ideally in a fully automated way, allowing to test a variety of observables in different models and in an effective field theory approach. In the process of achieving this goal we have developed an enhanced version of the tool Recola and on this basis the generalization Recola2. These tools represent fully automated tree- and one-loop-amplitude providers for the Standard Model, or in the case of Recola2 for general models. Concerning the algorithm, we use a purely numerical and fully recursive approach allowing for extreme calculations of yet unmatched complexity. Recola has led to the first computation involving 9-point functions. Beyond the Standard Model theories and Effective Field theories are integrated into the Recola2 framework as model files. Renormalized model files are produced with the newly developed tool Rept1l, which can perform the renormalization in a fully automated way, starting from nothing but Feynman rules. In view of validation, we have extended Recola2 to new gauges such as the Background-Field Method and the class of Rxi gauges. In particular, the Background-Field Method formulation for new theories serves as an automated validation, and is very useful in practical calculations and the formulation of renormalization conditions. We have applied the system to produce the first results for Higgs-boson production in Higgs strahlung and vector-boson fusion in the Two-Higgs-Doublet Model and the Higgs-Singlet Extension of the Standard Model. All in all, we have laid the foundation for an automated generation and computation of one-loop amplitudes within a large class of phenomenologically interesting theories. Furthermore, we enable the use of our system via a very flexible and dynamic control which does not require any intermediate intervention.}, subject = {Standardmodell }, language = {en} } @phdthesis{Herget2019, author = {Herget, Verena}, title = {A novel approach for the calibration of the hadronic recoil for the measurement of the mass of the W boson with the ATLAS Experiment}, doi = {10.25972/OPUS-17782}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-177828}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2019}, abstract = {The measurement of the mass of the \$W\$ boson is currently one of the most promising precision analyses of the Standard Model, that could ultimately reveal a hint for new physics. The mass of the \$W\$ boson is determined by comparing the \$W\$ boson, which cannot be reconstructed directly, to the \$Z\$ boson, where the full decay signature is available. With the help of Monte Carlo simulations one can extrapolate from the \$Z\$ boson to the \$W\$ boson. Technically speaking, the measurement of the \$W\$ boson mass is performed by comparing data taken by the ATLAS experiment to a set of calibrated Monte Carlo simulations, which reflect different mass hypotheses.\ A dedicated calibration of the reconstructed objects in the simulations is crucial for a high precision of the measured value. The comparison of simulated \$Z\$ boson events to reconstructed \$Z\$ boson candidates in data allows to derive event weights and scale factors for the calibration. This thesis presents a new approach to reweight the hadronic recoil in the simulations. The focus of the calibration is on the average hadronic activity visible in the mean of the scalar sum of the hadronic recoil \$\Sigma E_T\$ as a function of pileup. In contrast to the standard method, which directly reweights the scalar sum, the dependency to the transverse boson momentum is less strongly affected here. The \$\Sigma E_T\$ distribution is modeled first by means of its pileup dependency. Then, the remaining differences in the resolution of the vector sum of the hadronic recoil are scaled. This is done separately for the parallel and the pterpendicular component of the hadronic recoil with respect to the reconstructed boson. This calibration was developed for the dataset taken by the ATLAS experiment at a center of mass energy of \$8\,\textrm{TeV}\$ in 2012. In addition, the same reweighting procedure is applied to the recent dataset with a low pileup contribution, the \textit{lowMu} runs at \$5\,\textrm{TeV}\$ and at \$13\,\textrm{TeV}\$, taken by ATLAS in November 2017. The dedicated aspects of the reweighting procedure are presented in this thesis. It can be shown that this reweighting approach improves the agreement between data and the simulations effectively for all datasets. The uncertainties of this reweighting approach as well as the statistical errors are evaluated for a \$W\$ mass measurement by a template fit to pseudodata for the \textit{lowMu} dataset. A first estimate of these uncertainties is given here. For the pfoEM algorithm a statistical uncertainty of \$17\,\text{MeV}\$ for the \$5\,\textrm{TeV}\$ dataset and of \$18\,\text{MeV}\$ for the \$13\,\textrm{TeV}\$ are found for the \$W \rightarrow \mu \nu\$ analysis. The systematic uncertainty introduced by the resolution scaling has the largest effect, a value of \$15\,\text{MeV}\$ is estimated for the \$13\,\textrm{TeV}\$ dataset in the muon channel.}, subject = {Standardmodell }, language = {en} }