Conveners
Top Quark and Electroweak Physics: 1
- Tae Jeong Kim (Hanyang University (KR))
Top Quark and Electroweak Physics: 2
- Freya Blekman (IIHE, Vrije Universiteit Brussel (BE))
Top Quark and Electroweak Physics: 3
- Liang Han (University of Science and Technology of China (CN))
Top Quark and Electroweak Physics: 4
- Marcel Vreeswijk (Nikhef National institute for subatomic physics (NL))
Top Quark and Electroweak Physics: 5
- Jens Erler (IF-UNAM)
Top Quark and Electroweak Physics: 6
- Sahal Yacoob (University of Cape Town (ZA))
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Douglas John Paul Burns (University of Bristol (GB)), Douglas John Paul Burns (University of Bristol (GB))05/07/2018, 09:00Top Quark and Electroweak PhysicsParallel
Latest results on inclusive top quark pair production cross sections are presented using proton-proton collision data collected by CMS at different centre-of-mass energies, including 5 TeV. Final states with at least one charged lepton and one b-jet are explored to measure inclusive production cross sections. The sensitivity of some these measurements to PDFs and extraction of standard model...
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Peter Berta (Johannes Gutenberg Universitaet Mainz (DE))05/07/2018, 09:15Top Quark and Electroweak PhysicsParallel
Measurements of the inclusive and differential top-quark pair production cross sections in proton-proton collisions with the ATLAS detector at the Large Hadron Collider at center-of-mass energies of 8 TeV and 13 TeV are presented. The inclusive measurements reach high precision and are compared to the best available theoretical calculations. Differential measurements of the kinematic...
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Carlos Vazquez Sierra (Nikhef National institute for subatomic physics (NL))05/07/2018, 09:30Top Quark and Electroweak PhysicsParallel
LHCb, while purpose built for b-physics, also functions as a general purpose forward detector, covering the pseudo-rapidity range 2.0 to 5.0. Measurements of top production in the LHCb acceptance have particular sensitivity to high values of Bjorken-x, and offer complementary PDF constraints to measurements at the central detectors. In addition, the higher contribution from quark-initiated...
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Matthias Komm (Imperial College (GB))05/07/2018, 09:45Top Quark and Electroweak PhysicsParallel
Recent results on single top quark production are presented, performed using CMS data collected at different centre-of-mass energies. The single top quark analyses investigate separately the production of top quarks via t-channel exchange, in association with a W boson (tW) or via the s-channel. Differential measurements of t-channel production cross sections are also presented.
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Marcel Vreeswijk (Nikhef National institute for subatomic physics (NL))05/07/2018, 10:00Top Quark and Electroweak PhysicsParallel
Measurements of single top-quark production in proton-proton collisions and of angular correlations in single top-quark events are presented based on the 8 TeV and 13 TeV ATLAS datasets. For the production of single top quarks in the t-channel and the tW-channel, measurements of inclusive and differential cross-sections are included. Evidence for s-channel production using 8 TeV data and the...
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Bob Hirosky (University of Virginia (US))05/07/2018, 11:00Top Quark and Electroweak PhysicsParallel
We discuss the asymmetry between yields of forward- and backward-produced top and antitop quarks in $p\bar p \to t\bar t$ events at the Tevatron collider. These measurements use the full Run II data set in lepton plus jets and dilepton channels, recorded in the D0 and CDF detectors, corresponding to an integrated luminosity of $\approx 2\times10\ $fb$^{-1}$ . The combinations of inclusive and...
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Marisa Sandhoff (Bergische Universitaet Wuppertal (DE))05/07/2018, 11:15Top Quark and Electroweak PhysicsParallel
The large centre-of-mass energy available at the proton-proton collider LHC allows for the copious production of top quark pairs in association with other final state particles at high transverse momenta. The ATLAS experiment has measured several final state observables that are sensitive to additional radiation in top anti-top quark final states. Results on the top production in association...
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Nicolas Pierre Chanon (Centre National de la Recherche Scientifique (FR))05/07/2018, 11:30Top Quark and Electroweak PhysicsParallel
A comprehensive set of measurements of top quark pair and single top quark production in association with EWK bosons (W, Z or ɣ) is presented. The results are compared to theory predictions and re-interpreted as searches for new physics inducing deviations from the standard model predictions using an effective field theory approach. The status of the search for four top quark production, to...
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Alexander Josef Grohsjean (Deutsches Elektronen-Synchrotron (DE))05/07/2018, 11:45Top Quark and Electroweak PhysicsParallel
Top quark production can probe physics beyond the SM in different ways. Some processes, and especially certain angular correlations, are sensitive to the existence of anomalous top quark couplings. In the SM, flavour-changing neutral currents (FCNC) are forbidden at tree level and are strongly suppressed in loop corrections. Several extensions of the SM incorporate significantly enhanced FCNC...
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Dr Ligang Xia (University of Warwick (GB))05/07/2018, 12:00Top Quark and Electroweak PhysicsParallel
The top quark is the heaviest known fundamental particle and probing its couplings with the other fundamental particle may open a window to physics beyond the Standard Model. Searches for flavour-changing neutral current top-quark interactions are discussed based on the 13 TeV ATLAS dataset. Searches for rare top quark decays to Higgs and Z bosons are presented in top quark pair production,...
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Prof. Bennie Ward (Baylor University), Bennie Ward (Baylor University (US))05/07/2018, 16:30Top Quark and Electroweak PhysicsParallel
KKMC-hh is a precision event-generator for Z production and decay in hadronic collisions, which
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applies amplitude-level resummation to both initial and final state photon radiation, including
perturbative residuals exact through order $\alpha^2L$, together with exact order $\alpha$ electroweak matrix element corrections. We present some comparisons to other programs and results showing the... -
Zhiqing Philippe Zhang (LAL, Orsay (FR))05/07/2018, 17:00Top Quark and Electroweak PhysicsParallel
An improved determination of electroweak (EW) parameters using H1 inclusive neutral current and charged current DIS cross sections is presented. The analysis benefits from the usage of the previously published cross sections using longitudinally polarised lepton beams. The parameters are determined in a combined fit of EW parameters together with PDFs. The predictions include NNLO QCD...
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Kenneth Long (University of Wisconsin Madison (US))05/07/2018, 17:15Top Quark and Electroweak PhysicsParallel
The production of massive vector boson pairs is a key process for the understanding of the non-abelian gauge structure of the standard model and for the comprehension of the electroweak symmetry breaking mechanism. The study of the production of vector boson pairs with the presence of two jets in the event allows to measure the electroweak production of vector bosons in association with jets,...
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Rustem Ospanov (University of Science and Technology of China)05/07/2018, 17:30Top Quark and Electroweak PhysicsParallel
Measurements of the cross sections of the production of pairs of electroweak gauge bosons at the LHC constitute stringent tests of the electroweak sector and provide model-independent means to search for new physics at the TeV scale. Similarly, the electroweak production of vector bosons in proton-proton collisions tests the gauge structure of the Standard Model. The ATLAS collaboration has...
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Marc-Andre Pleier (Brookhaven National Laboratory (US)), Marc-Andre Pleier (Brookhaven National Laboratory (US))05/07/2018, 17:45Top Quark and Electroweak PhysicsParallel
Measurements of the cross sections of the production of three electroweak gauge bosons and of vector-boson scattering processes at the LHC constitute stringent tests of the electroweak sector of the Standard Model and provide a model-independent means to search for new physics at the TeV scale. The ATLAS collaboration searched for the production of three W bosons or of a W boson and a photon...
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Riccardo Bellan (Universita e INFN Torino (IT))05/07/2018, 18:00Top Quark and Electroweak PhysicsParallel
Precision measurements of multi-boson production is a validation of the Standard Model. These multi-boson processes are a background to Higgs measurements and searches for Beyond the Standard Model physics. In this talk, we present the recent measurements of multiboson final states performed in CMS, involving W, Z and photon combinations. Inclusive and differential cross sections are compared...
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Jürgen Reuter (DESY Hamburg, Germany)05/07/2018, 18:15Top Quark and Electroweak PhysicsParallel
The International Linear Collider is now proposed with a staged machine design, with the first stage at sqrt(s)=250 GeV and an integrated luminosity goal of 2 ab^-1. One of the questions for the machine design is the importance of positron polarization. In this report, we review the impact of positron polarization on the physics goals of the 250 GeV stage of the ILC and demonstrate that...
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David Miller (University of Glasgow)06/07/2018, 11:00Top Quark and Electroweak PhysicsParallel
We will describe the latest TopFitter analysis, which uses top quark observables to fit the Wilson Coefficients of the SM augmented with dimension 6 operators. In particular, we will discuss the inclusion of new LHC Run II data, and the implementation of particle-level observables.
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Oleksandr Zenaiev (DESY)06/07/2018, 11:30Top Quark and Electroweak PhysicsParallel
State-of-the-art theoretical predictions accurate to next-to-leading order QCD interfaced with Pythia8, Herwig, and Sherpa event generators are tested by comparing the unfolded ttbar differential data collected with the CMS detector at 8 and 13 TeV. These predictions are also compared with the underlying event activity distributions in ttbar events using CMS proton-proton data collected at a...
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Reinhild Peters (University of Manchester (GB))06/07/2018, 11:45Top Quark and Electroweak PhysicsParallel
The top quark is the heaviest known fundamental particle. As it is the only quark that decays before it hadronizes, this gives the unique opportunity to probe the properties of bare quarks. This talk will focus on a few recent precision measurements of top quark properties in production and decay by the ATLAS Collaboration at center-of-mass energies of 8 TeV and 13 TeV.
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Prof. Chung Kao (University of Oklahoma)06/07/2018, 12:00Top Quark and Electroweak PhysicsParallel
We investigate the prospects for discovering a top quark decaying into
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one light Higgs boson along with a charm quark in top quark pair production
at the CERN Large Hadron Collider (LHC) and future hadron colliers.
A general two Higgs doublet model is adopted to study the signature
of flavor changing neutral Higgs (FCNH) interactions with $t \to c\phi^0$,
followed by $\phi^0 \to b\bar{b},... -
Ulrike Schnoor (CERN)06/07/2018, 12:15Top Quark and Electroweak PhysicsParallel
The Compact Linear Collider (CLIC) is a mature option for a future electron-positron collider operating at centre-of-mass energies of up to 3 TeV. CLIC will be built and operated in a staged approach with three centre-of-mass energy stages currently assumed to be 380 GeV, 1.5 TeV and 3 TeV. This talk discusses the prospects for top-quark physics at the two TeV-scale CLIC energy stages based on...
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Siqi Yang (The University of Iowa (US))06/07/2018, 16:30Top Quark and Electroweak PhysicsParallel
We present the measurements of forward-backward charge asymmetry $A_{FB} $ in
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$p\bar{p}\rightarrow Z/\gamma^{*} \rightarrow \mu^+\mu^- $ events using $9.7 \ $fb$^{-1}$ of $ p\bar p$ data collected at $\sqrt s=1.96\ $TeV by the D0 detector at the Fermilab Tevatron collider. $A_{FB}$ is measured as a function of the invariant mass of the dimuon system to extract the effective weak mixing... -
Prof. Liang Han (University of Science and Technology of China (CN))06/07/2018, 16:45Top Quark and Electroweak PhysicsParallel
We combine four measurements of the forward-backward charge asymmetry $A_{FB} $ in
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$p\bar{p}\rightarrow Z/\gamma^{*} \rightarrow e^+ e^-/\mu^+\mu^- + X$ events using $\sim 10\ $fb$^{-1}$ of $ p\bar p$ data collected at $\sqrt s=1.96\ $TeV by the CDF and D0 detectors at the Fermilab Tevatron collider. $A_{FB}$ is measured as a function of the invariant mass of the dilepton system to extract... -
Ilya Gorbunov (Joint Institute for Nuclear Research (RU))06/07/2018, 17:00Top Quark and Electroweak PhysicsParallel
Measurements of single W and Z boson inclusive and differential production cross sections with the CMS detector are presented. Measurements of Drell-Yan cross sections in the mass range of 15 to 3000 GeV are also reported. The results are compared to predictions from different Monte Carlo generators.
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Manuella Vincter (Carleton University (CA))06/07/2018, 17:15Top Quark and Electroweak PhysicsParallel
Precision measurements of the Drell-Yan production of Z bosons at the LHC provide a benchmark of our understanding of perturbative QCD and electroweak processes and probe the proton structure in a unique way. ATLAS performed a precise triple differential Drell-Yan cross-section measurement as a function of Mll, dilepton rapidity and cosθ∗ defined in the Collins-Soper frame at a center of mass...
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Pavel Krokovny (Budker Institute of Nuclear Physics (RU))06/07/2018, 17:30Top Quark and Electroweak PhysicsParallel
A variety of vector boson measurements have been performed at LHCb with Run 1 data, including inclusive Z/W cross-sections, the Z forward-backward asymmetry, Z/W production with jets (including heavy flavor). Additionally, the inclusive Z cross-sections have been measured with Run 2 data. A variety of these results will be presented.
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Sviatoslav Bilokin (Université Paris-Saclay (FR)), Sviatoslav Bilokin (Institut Pluridisciplinaire Hubert CURIEN)06/07/2018, 17:45Top Quark and Electroweak PhysicsParallel
The 3rd generation quarks are, due to their large mass, highly sensitive probes for new physics connected to the electroweak symmetry breaking. While top quark pair production requires center-of-mass energies of larger than 350 GeV, the first stage of the ILC at a center-of-mass energy of 250 GeV can perform precision measurements of bottom quark pair production, thereby settling the long...
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Prof. Zhijun Liang (Chinese Academy of Sciences (CN))06/07/2018, 18:00Top Quark and Electroweak PhysicsParallel
Abstract: The Circular Electron Positron Collider (CEPC) project aims to build a circular electron-positron collider capable of precision physics measurements at center-of-mass energies ranging from 90 GeV to 240GeV. The CEPC has a total circumference of at least one hundred kilometers and at least two interaction points. In its 10 years operation at 240 GeV, it will collect more than one...
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Tadeusz Lesiak (Polish Academy of Sciences (PL))06/07/2018, 18:15Top Quark and Electroweak PhysicsParallel
The Future Circular Collider with electron-positron beams (FCC-ee) should provide improvements of the electroweak precision measurement concerning Z, W, H and their masses by a large factor over the present status.
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The unparalleled experimental precision would open, via Electroweak loop corrections, a broad discovery potential for new, at least weakly interacting particles up to high energy... -
Jürgen Reuter (DESY Hamburg, Germany)07/07/2018, 16:30Top Quark and Electroweak PhysicsParallel
The threshold scan at future lepton colliders is the most precise
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known method to determine the top quark mass (well below 100 MeV), a
fundamental parameter of the Standard Model that co-determines the
stability properties of the electroweak vacuum. We present a new method to
match the continuum next-to-leading order QCD corrections with the
next-to-leading logarithmic resummation of the... -
Stefan Soldner-Rembold (University of Manchester (GB))07/07/2018, 17:00Top Quark and Electroweak PhysicsParallel
We discuss extractions of the pole mass of the top quark based on measurements of the inclusive and unfolded differential $p\bar p \to t\bar t$ production cross section as a function of $p_T(t)$ and $M(t\bar t)$. We use the full Run II (2001--2011) data set of $p \bar p$ collisions at $\sqrt s=1.96 $TeV collected by the D0 experiment, corresponding to an integrated luminosity of $9.7...
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Teresa Barillari (Max-Planck-Institut fur Physik (DE))07/07/2018, 17:15Top Quark and Electroweak PhysicsParallel
The top quark mass is one of the fundamental parameters of the Standard Model. The latest ATLAS measurements of the top quark mass in top quark pair final states are presented. Measurements use dilepton, lepton+jets and all-hadronic final states and their combination is performed. Measurements of the top quark pole mass based on precision theoretical QCD calculations for lepton kinematic...
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Nataliia Kovalchuk (Hamburg University (DE))07/07/2018, 17:30Top Quark and Electroweak PhysicsParallel
Measurements of top quark properties using data collected by the CMS experiment at 13 TeV are presented. The top quark mass is measured in the lepton+jets channel is consistent with the CMS measurements of Run-1. The top quark mass is also studied as a function of the event kinematical properties. For the first time at the LHC, the width of the top quark is directly probed during Run-2, in...
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Alexander Savin (University of Wisconsin Madison (US))07/07/2018, 17:45Top Quark and Electroweak PhysicsParallel
The High-Luminosity Large Hadron Collider (HL-LHC) is expected to deliver an integrated luminosity of up to 3000 fb-1. The very high instantaneous luminosity will lead to about 200 proton-proton collisions per bunch crossing (“pileup”) superimposed to each event of interest, therefore providing extremely challenging experimental conditions. Prospects for selected Standard Model (SM)...
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Aleksander Zarnecki (University of Warsaw (PL))07/07/2018, 18:00Top Quark and Electroweak PhysicsParallel
The Compact Linear Collider (CLIC) is a mature option for a future electron-positron collider operating at centre-of-mass energies of up to 3 TeV. CLIC will be built and operated in a staged approach with three centre-of-mass energy stages currently assumed to be 380 GeV, 1.5 TeV and 3 TeV. This talk discusses the prospects for precision measurements of the top-quark properties at the first...
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Clement Helsens (CERN)07/07/2018, 18:15Top Quark and Electroweak PhysicsParallel
The FCC-ee project includes a running time at and above the top pair production threshold.
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The collection of about 0.2 ab-1 at the tt threshold would allow the most precise measurement of the top mass with about 10 MeV of statistical accuracy. The threshold region can also be used to measure the top width and extract an indirect value of the top Yukawa coupling. A second running phase will...