27–31 Aug 2018
TU Dresden
Europe/Zurich timezone

Contribution List

107 out of 107 displayed
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  1. 27/08/2018, 09:00
  2. Klaus Rabbertz (KIT - Karlsruhe Institute of Technology (DE))
    27/08/2018, 09:10
  3. Robert Samuel Thorne (University College London (UK))
    27/08/2018, 10:05
  4. Andre Hoang (University of Vienna)
    27/08/2018, 11:30
  5. Till Michael Arndt (Deutsches Elektronen-Synchrotron (DE))
    27/08/2018, 12:15
  6. Stefano Di Vita (Università degli Studi e INFN Milano (IT))
    27/08/2018, 14:30
    Perturbative QCD, Jets and Substructure

    Multi-loop Feynman integrals represent an essential building block for the precision physics program at high-energy colliders and beyond. In my talk I will review recent developments concerning their evaluation with the method of differential equations, giving particular emphasis to the so-called canonical form and presenting some examples of phenomenological interest.

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  7. Markus Diehl (DESY)
    27/08/2018, 14:30
    PDFs, 𝛼ₛ and soft QCD

    I review the theory status of double parton scattering, with emhasis on higher-order raditative corrections.

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  8. Andrzej Konrad Siodmok (Polish Academy of Sciences (PL))
    27/08/2018, 14:30
  9. Knut Zoch (Georg August Universitaet Goettingen (DE))
    27/08/2018, 14:30
    Heavy Quarks

    Measurements of the inclusive and differential cross-sections for top-quark pair and single top production cross sections in proton-proton collisions with the ATLAS detector at the Large Hadron Collider are presented at center-of-mass energies of 8 TeV and 13 TeV. The inclusive measurements reach high precision and are compared to the best available theoretical calculations. These...

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  10. Ulrich Schubert (Argonne National Laboratory)
    27/08/2018, 15:00
    Perturbative QCD, Jets and Substructure

    The calculation of Feynman Integrals is one of bottlenecks for precision calculations at Next-to-Next-to-leading order and beyond. Differential Equations have proven to be a powerful tool to relieve this bottleneck and have seen a rapid development in the last years. In this talk I will review these recent developments especially focusing on the so-called canonical form. I will present the...

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  11. Federico Buccioni (University of Zurich)
    27/08/2018, 15:00
    Heavy Quarks

    Precise measurements of Higgs boson production in association with top-quark pairs
    allow for constraints on the top-quark Yukawa coupling, which in turn is crucial to fully
    characterise the scalar sector of the Standard Model and could also open a window on
    Beyond-the-Standard-Model interactions. At the Large Hadron Collider, searches for
    $t\bar{t}H$ production in the dominant $H \to b...

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  12. Alexander Glazov (Deutsches Elektronen-Synchrotron (DE))
    27/08/2018, 15:00
    PDFs, 𝛼ₛ and soft QCD

    We present the xFitter project  which provides an open-source software framework
    for the determination of the proton's  parton distribution functions and for the interpretation of the physics analyses in the context of  Quantum Chromodynamics.
    The project has been used recently for a number of analyses performed by the LHC collaborations and theory community, which are summarised briefly. The...

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  13. Davide Pagani (TUM - Garching bei München)
    27/08/2018, 15:00
    Monte Carlo and Resummation

    We discuss the automation of the calculation of leading- and next-to-leading order contributions to short-distance cross sections at hadron colliders. With the new public version of the code MadGraph5_aMC@NLO, not only NLO QCD and EW corrections but also all the subleading contributions in a mixed QCD and EW coupling expansion can now be calculated. We discuss the key features for obtaining...

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  14. Anna Katarzyna Kulesza (Westfaelische Wilhelms-Universitaet Muenster (DE))
    27/08/2018, 15:30
    Heavy Quarks

    The investigation of the $pp \rightarrow t {\overline t} H$ process is among the highest priorities of the current LHC physics program. Correspondingly, improvements in precision with which theoretical predictions for this process are known are of central importance. In this talk the recent progress concerning theoretical predictions for the signal will be reviewed.

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  15. Daniel Britzger (Max-Planck-Institut für Physik München)
    27/08/2018, 15:30
    PDFs, 𝛼ₛ and soft QCD

    Calculations for dijet production in diffractive deep-inelastic scattering (DIS) at next-to-next-to-leading order accuracy (NNLO) are presented. The calculations are based on the antenna subtraction formalism and the hard coefficients are convoluted with currently available PDFs for diffractive scattering (DPDFs).
    The NNLO predictions are compared to a large number of available measurements...

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  16. Enrico Bothmann (University of Edinburgh)
    27/08/2018, 15:30
    Monte Carlo and Resummation

    In this status report on the multi-purpose Monte-Carlo event generator Sherpa
    I review recent and ongoing Sherpa studies, as well as the latest
    developments of its fixed-order and all-order technologies. Fixed-order
    improvements I discuss include fully automated EW corrections and support
    for additional loop-induced processes. On the all-order side I cover
    Sherpa's parton showers and the...

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  17. Mr Daniel Hulme (UZH)
    27/08/2018, 15:30
    Perturbative QCD, Jets and Substructure

    Abstract: An algorithm for the systematic analytical approximation of multi-scale Feyn-
    man integrals will be discussed. The algorithm produces algebraic expressions as functions of
    the kinematical parameters and mass scales appearing in the Feynman integrals, allowing
    for fast numerical evaluation. The results are valid in all kinematical regions, both above
    and below thresholds, up to in...

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  18. Eram Syed Rizvi (Queen Mary, University of London)
    27/08/2018, 16:30
    EW, Higgs and BSM

    The parameters of the electroweak theory are determined in a combined electroweak and QCD analysis using all deep-inelastic $e^+p$ and $e^-p$ neutral current and charged current scattering cross sections published by the H1 Collaboration, including data with longitudinally polarised lepton beams. The mass of the $W$ boson in the on-shell scheme is determined as $\mW=80.508\pm 0.115\,\GeV$. The...

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  19. Mario Jose Sousa (Shandong University (CN))
    27/08/2018, 16:30
    Monte Carlo and Resummation

    A number of Higgs measurements and searches for new phenomena in the Higgs sector rely on identification or vetos of particle jets with fairly low transverse momentum in the range of 20-30 GeV. In these cases uncertainties from the modelling of the parton shower and the underlying event can be sizeable. This talk will give an overview of how these uncertainties enter in several analyses.

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  20. Marius Wiesemann (CERN)
    27/08/2018, 16:30
    Perturbative QCD, Jets and Substructure

    I will review recent theory developments for diboson production at the LHC within the puclicly available code MATRIX: With the two lepton plus two neutrino channels, which mix ZZ and WW production, NNLO corrections have been completed to all experimentally relevant leptonic final states for diboson processes. NLO corrections to the loop-induced gg channel are formally of N3LO accuracy, but...

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  21. Thorsten Kuhl (Deutsches Elektronen-Synchrotron (DE))
    27/08/2018, 16:50
    Monte Carlo and Resummation

    Abstract will be available shortly. The talk has been suggested by the organizer
    ATLAS + CMS.
    The content of this talk is related to the activities of one the CMS groups (Generator, Forward, SM, Top) and ATLAS groups (PMG, SM, TOP, Forward).

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  22. Marco Bonetti (Karlsruhe Institute of Technology (KIT))
    27/08/2018, 16:53
    EW, Higgs and BSM

    The study of the Higgs boson properties is one of the main tasks of contemporary high-energy physics. Among Higgs properties, its interaction with gluons is interesting since it can be facilitated by yet unknown elementary particles. One of the major sources of uncertainty in the theoretical description of $ggH$ coupling originates from mixed QCD-electroweak contributions. The NLO QCD...

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  23. Jonathan Crane (University of Manchester (GB))
    27/08/2018, 17:00
    Perturbative QCD, Jets and Substructure

    Measurements of the cross sections of the production of two or three electroweak gauge bosons 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. Such studies can be complemented by measurements of vector boson fusion or vector boson scattering processes with one or two gauge...

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  24. Kirill Kudashkin (Karlsruhe Institute of Technology (KIT))
    27/08/2018, 17:16
    EW, Higgs and BSM

    In this talk I will present our results on the Higgs plus jet production at the large transverse momentum, that is, above the top mass threshold. In particular, it will be shown how corresponding two-loop amplitudes were computed in approximation of nearly massless top quarks.

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  25. Andreas Hinzmann (Hamburg University (DE))
    27/08/2018, 17:30
    Perturbative QCD, Jets and Substructure

    Precise measurements of the mass of the W boson are important to test the overall consistency of the Standard Model of particle physics. The current best measurements of the W boson mass come from single production measurements at hadron colliders in its decay mode to a lepton (electron or muon) and a neutrino and pair production of W bosons at lepton colliders, where also the decay mode of...

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  26. Junya Nakamura (Universität Tübingen)
    27/08/2018, 17:39
    EW, Higgs and BSM

    In this talk I show that the $Z$ boson polarization has relevant information to distinguish the signal $pp \to ZH$, $H \to b\bar{b}$ from the dominant background $Zb\bar{b}$, which is part of the $\mathcal{O}(\alpha_s^2)$ correction to the Drell-Yan $Z$ production, and can help us to finally observe the largest Higgs boson branching ratio.

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  27. Jonas Lindert (University of Durham (GB)), Paolo Gunnellini (University of Hamburg)
    28/08/2018, 09:00
  28. Anna Kulesza (University of Muenster)
    28/08/2018, 10:15
  29. Dezso Horvath (Wigner RCP, Budapest (HU))
    28/08/2018, 11:30
  30. Livio Bianchi (Universita e INFN Torino (IT))
    28/08/2018, 12:15
  31. Frederic Alexandre Dreyer (MIT)
    28/08/2018, 14:30
    Monte Carlo and Resummation
  32. Daniel Britzger (Ruprecht Karls Universitaet Heidelberg (DE))
    28/08/2018, 14:30
    PDFs, 𝛼ₛ and soft QCD

    The strong coupling constant $\alpha_s$ is determined from inclusive jet and dijet cross sections in neutral-current deep-inelastic ep scattering (DIS) measured at HERA by the H1 collaboration using next-to-next-to-leading order (NNLO) QCD predictions. The dependence of the NNLO predictions and of the resulting value of $\alpha_s(m_Z)$ at the $Z$-boson mass $m_Z$ are studied as a function of...

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  33. Paul Glaysher (DESY)
    28/08/2018, 14:30

    After the discovery of the Higgs boson in summer 2012, the understanding its properties has been a high priority of the ATLAS physics program. Measurements of Higgs boson properties sensitive to its production processes, decay modes, kinematics, mass, and spin/CP properties based on pp collision data recorded at 13 TeV are presented. The analyses in several decay channels will be described and...

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  34. Heribertus Bayu Hartanto (Durham University)
    28/08/2018, 14:30
    Perturbative QCD, Jets and Substructure

    I will present a calculation of the leading-colour five-gluon amplitude at two loop in QCD. The calculation is performed by means of D-dimensional integrand reduction method, complemented with the finite-field reconstruction techniques and momentum twistor parameterization. Numerical results for all helicity configurations are obtained by employing both sector decomposition methods and IBP...

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  35. Mr Wojciech Bizon (University of Oxford (GB))
    28/08/2018, 14:52
    Monte Carlo and Resummation

    We present a direct space resummation formalism for colour singlet production in hadronic collisions. We focus on N3LL results for Higgs boson production in gluon-gluon fusion as well as results for Drell-Yan production, we show predictions with phenomenological cuts matched to NNLO fixed-order predictions.

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  36. Mathieu Pellen (University Wuerzburg)
    28/08/2018, 14:53
    EW, Higgs and BSM

    In this talk, I review recent theoretical developments for VBS processes at the LHC.

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  37. Daniel Maitre
    28/08/2018, 14:55
    PDFs, 𝛼ₛ and soft QCD

    I will present a strong coupling constant extraction at next-to-leading order QCD accuracy using ATLAS Z+2,3,4 jets data. This is the first extraction using processes with a dependency on high powers of the coupling constant. The values of the strong coupling constant at the Z mass obtained are compatible with the world average and with uncertainties commensurate with other next-to-leading...

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  38. Adam Kardos (University of Debrecen)
    28/08/2018, 15:00
    Perturbative QCD, Jets and Substructure

    We observe more and more advances in the technology of multiloop calculations.
    Hence it is of utmost importance to develope computational frameworks which
    can tackle the computational burden presented by the regularization
    of up to two unresolved parton emissions coming from the matrix elements.
    CoLoRFulNNLO is such a framework built around local subtractions
    derived from first principles. In...

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  39. Andreas Maier (Durham University)
    28/08/2018, 15:14
    Monte Carlo and Resummation

    The weak boson fusion contribution to Higgs boson production is enhanced significantly by requiring a large invariant mass and rapidity separation between the associated jets. This induces large logarithmic corrections in the prediction for the gluon-fusion background, which are incorporated to all orders within the High Energy Jets (HEJ) formalism. We present HEJ predictions for the...

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  40. Stefano Camarda (Johannes Gutenberg Universitaet Mainz (DE))
    28/08/2018, 15:15
    PDFs, 𝛼ₛ and soft QCD

    The strong-coupling constant $\alpha_s(m_Z)$ is measured from the transverse momentum distribution of Z bosons measured at $\sqrt{s} = 1.96$ TeV with the CDF experiment, using predictions based on qt resummation at NNLO+NNLL, as implemented in the DYTURBO program. The measurement is performed through a simultaneous fit of $\alpha_s(m_Z)$, PDFs, and the non-perturbative Sudakov form factor.

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  41. Jakob Salfeld-Nebgen (Princeton University (US))
    28/08/2018, 15:16
    EW, Higgs and BSM

    This talk describe recent results on the measurement of the Electroweak production of V and VV + jets.

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  42. Mr Suman Chatterjee (Tata Inst. of Fundamental Research (IN))
    28/08/2018, 15:30
    Perturbative QCD, Jets and Substructure

    We present measurements of differential jet cross sections over a wide range in transverse momenta from inclusive jets to multi-jet final states. Studies on the impact that these measurements have on the determination of the strong coupling alpha_s as well as on parton density functions are reported.

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  43. Daniel Savoiu (KIT - Karlsruhe Institute of Technology (DE))
    28/08/2018, 15:35
    PDFs, 𝛼ₛ and soft QCD

    https://arxiv.org/abs/1712.00480

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  44. Simone Marzani (Università di Genova and INFN Genova)
    28/08/2018, 15:36
    Monte Carlo and Resummation
  45. Wenhao Xu (University of Michigan (US))
    28/08/2018, 15:39
    EW, Higgs and BSM

    New Results on Vector Boson Scattering Processes with the ATLAS Detector

    Measurements of the cross sections of the 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 observed the electroweak production of WZ and...

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  46. Malin Sjodahl (Lund University)
    28/08/2018, 16:30
    Monte Carlo and Resummation
  47. Jan Niehues
    28/08/2018, 16:30
    Perturbative QCD, Jets and Substructure

    In this talk, recent results on the calculation of fully differential single-jet production in neutral current deep inelastic scattering at next-to-next-to-next-to leading order (N3LO) in the strong coupling are presented. The results are obtained by the combination of antenna subtraction at next-to-next-to leading order (NNLO) with the method of projection to born. Details of the combination...

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  48. Francesco Brivio (Universita & INFN, Milano-Bicocca (IT))
    28/08/2018, 16:30
    EW, Higgs and BSM

    The production of Higgs boson pairs (HH) offers a unique opportunity to explore the structure of the Higgs field potential through the determination of the Higgs boson self interaction. Despite being an extremely rare process, with a predicted cross section of about 33 fb at a center-of-mass energy of 13 TeV, variations of the Higgs couplings, or the presence of heavy resonances, might enhance...

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  49. Jan Piclum (University of Siegen)
    28/08/2018, 16:30
    Heavy Quarks

    The total top-antitop production cross section at hadron colliders is
    one of the key observables of the Standard Model. Comparisons of LHC
    measurements with theoretical calculations are being used to determine
    the top-quark mass and the strong coupling and are included in global
    PDF fits. These applications are currently based on calculations at
    the next-to-next-to-leading order (NNLO) in QCD...

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  50. Patrick Kirchgaesser
    28/08/2018, 16:52
    Monte Carlo and Resummation

    We consider soft gluon evolution of a system of clusters forming the initial state of the cluster hadronziation model, in order to constrain colour reconnection models from a perturbative point of view.
    We show that this ansatz produces clusters with properties attributed to
    a colour pre-confined state and find strong evidence for formerly investigated colour reconnection models based on...

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  51. Ludovic Michel Scyboz (Max-Planck-Institut fur Physik (DE))
    28/08/2018, 16:53
    EW, Higgs and BSM
  52. Felix Ringer (Lawrence Berkeley National Laboratory)
    28/08/2018, 17:00
    Perturbative QCD, Jets and Substructure

    The phenomenology of highly energetic jets and their substructure plays an important role for the physics program at the LHC. In recent years various grooming techniques have been proposed that need to be included consistently in perturbative calculations. Within Soft Collinear Effective Theory (SCET) we establish factorization theorems for jet substructure observables measured on an inclusive...

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  53. Kevin De Vasconcelos Corga (Centre National de la Recherche Scientifique (FR))
    28/08/2018, 17:00
    Heavy Quarks

    The top quark is unique among the known quarks in that it decays before it has an opportunity to form hadronic bound states. This makes measurements of its properties particularly interesting as one can access directly the properties of a bare quark. The latest measurements of these properties with the ATLAS detector at the LHC are presented using 8 TeV and 13 TeV data. Limits on the rate of...

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  54. Sebastian Liebschner (IKTP Dresden)
    28/08/2018, 17:14
    Monte Carlo and Resummation

    NLO-subtraction schemes such as CS-dipole-subtraction are indispensable for MC-Generators to calculate real and virtual corrections efficiently. However, those algorithms suffer from numerical inefficiencies and even cause distortions in physical distributions when interfaced with parton showers, if the process in question comprises potentially resonant particles.
    In this talk I will elucidate...

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  55. Pawel Jan Klimek (Northern Illinois University (US))
    28/08/2018, 17:16
    EW, Higgs and BSM

    Several theories beyond the Standard Model predict the existence of additional neutral or charged Higgs particles, as well as decays of the Higgs boson that are either forbidden or strongly suppressed in the SM.Results from selected recent searches for additional Higgs bosons in different production processes and decay modes, and for BSM decays of the 125 GeV-Higgs boson will be presented.

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  56. Torsten Weber (RWTH Aachen University)
    28/08/2018, 17:30
    Heavy Quarks

    We present a complete description of top quark pair production in association with a hard photon in the dilepton channel. Our calculation is accurate to NLO in QCD. It is based on matrix elements for e+νeμ−ν¯μbb¯γ production and includes all resonant and non-resonant diagrams, interferences, and off-shell effects of the top quarks and the W gauge bosons. This calculation constitutes the first...

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  57. Robin Cameron Aggleton (Hamburg University (DE))
    28/08/2018, 17:30
    Perturbative QCD, Jets and Substructure

    Jets are the experimental signature of energetic quarks and gluons produced in high energy processes. A detailed understanding of both the energy scale and the transverse momentum resolution of jets is of crucial importance for the analysis of perturbative QCD processes. In addition, the substructure, shape and mass of jets is an important tool to separate and study quark and gluon initiated...

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  58. Dr Leonardo Vernazza (Nikhef and University of Amsterdam)
    28/08/2018, 17:36
    Monte Carlo and Resummation

    I will discuss recent developments in the calculation of next-to-leading power corrections in Drell Yan and other electroweak annihilation processes.

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  59. Matthias Saimpert (Deutsches Elektronen-Synchrotron (DE))
    28/08/2018, 17:39
    EW, Higgs and BSM

    QCD Issues in Searches for New Physics with the ATLAS Detector

    The ATLAS experiment at the LHC has a broad search program covering a wide variety of models of physics beyond the Standard Model, from simplified models to UV complete models like supersymmetry. In many searches, the final states include one or more hadronic object, and QCD constitutes a crucial background, the control and...

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  60. Aparajita Dattagupta (University of Oregon (US))
    29/08/2018, 09:00
  61. Bogdan Malaescu (Centre National de la Recherche Scientifique (FR) & CERN), Joao Pires
    29/08/2018, 09:45
  62. Stephen Jones (MPI, Munich)
    29/08/2018, 11:30
  63. Marek Schoenherr (CERN)
    29/08/2018, 12:15
  64. Danilo Enoque Ferreira De Lima (Ruprecht Karls Universitaet Heidelberg (DE)), Dr Simone Marzani (Università di Genova and INFN Genova)
    30/08/2018, 09:45
  65. Stefano Forte (Università degli Studi e INFN Milano (IT))
    30/08/2018, 11:30
  66. Nicola Anne Skidmore (Ruprecht Karls Universitaet Heidelberg (DE))
    30/08/2018, 12:15
  67. Christoph Michael Langenbruch (Rheinisch Westfaelische Tech. Hoch. (DE))
    30/08/2018, 14:30
    Heavy Quarks

    Rare decays are powerful probes for Physics beyond the Standard Model
    (SM), as new particles can have a large impact on physics observables.
    Recent results on lepton universality tests and measurements of
    branching fractions and angular distributions of rare b->sll decays have
    shown tensions with the SM predictions. The LHCb experiment is ideally
    suited for the study of the these flavour...

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  68. Serguei Alekhin (State Res.Center of Russian Feder. Inst.f.High Energy Phys. (IFVE))
    30/08/2018, 14:30
    PDFs, 𝛼ₛ and soft QCD

    Results of the QCD analysis of a variety of the hard-scattering data is overviewed with a particular focus on determination of the quark distributions in the nucleon. A potential of the recent precise data collected at the LHC for the problem of parton species disentangling is discussed and compared to the impact of the low-energy fixed-target data. Finally, remaining challenges and potential...

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  69. Andrzej Konrad Siodmok (Polish Academy of Sciences (PL))
    30/08/2018, 14:30
    Monte Carlo and Resummation
  70. Frederic Alexandre Dreyer (MIT)
    30/08/2018, 14:30
    Perturbative QCD, Jets and Substructure

    Lund diagrams, a representation of the phase space within jets, have long been used in discussing parton showers and resummations. I will point out that they can also serve as a powerful tool for experimentally characterising the radiation pattern within jets. I will briefly comment on some of their analytical properties and highlight their scope for constraining Monte Carlo simulations. I...

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  71. Andre Hoang (University of Vienna)
    30/08/2018, 14:52
    Monte Carlo and Resummation
  72. Eram Syed Rizvi (Queen Mary, University of London)
    30/08/2018, 15:00
    PDFs, 𝛼ₛ and soft QCD

    The talk should cover W, Z/gamma* measurements sensitive to PDFs, as well as measurements of EW observables which are affected by significant PDF uncertainties (sin2thetaW, W mass).

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  73. Danny van Dyk (TU München)
    30/08/2018, 15:00
    Heavy Quarks

    I will discuss recent developments regarding long-distance effects in B->K(*)l+ l- decays.
    Precise knowledge of these effects is needed for the interpretation of the present anomaly seen in the experimental results. The approach I discuss relies on the analytic properties of the hadronic matrix elements. It combines the available theory information beyond the physical phase space with...

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  74. Ana Rosario Cueto Gomez (Universidad Autonoma de Madrid (ES))
    30/08/2018, 15:00
    Perturbative QCD, Jets and Substructure

    The production of prompt isolated photons at hadron colliders provides a stringent test of perturbative QCD and can be used to probe the gluon density function of the proton.
    The ATLAS collaboration has performed numerous cross section measurements of prompt photon production, among which are a precise measurement of the production of isolated prompt photons in association with heavy flavor...

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  75. Daniel Reichelt (Technische Universitaet Dresden (DE))
    30/08/2018, 15:14
    Monte Carlo and Resummation
  76. Dr Keri Vos (Siegen University)
    30/08/2018, 15:30
    Heavy Quarks

    The search for CP violation is a large part of the flavour programs at LHCb and the B factories, with pure hadronic decays as the key players. Three-body decays, which form a large part of the B meson branching fraction, contain much more information than two-body decays, because of their non-trivial kinematic structure. Recently, these decays were described using a QCD factorization framework...

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  77. Peter Wagner (University of Bonn (DE))
    30/08/2018, 15:30
    Perturbative QCD, Jets and Substructure

    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 measurement of the effective leptonic weak mixing angle using electron and muon pairs from Z boson decay at a center of mass energy of 8 TeV. It consists of a set of...

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  78. Suman Chatterjee (Tata Inst. of Fundamental Research (IN))
    30/08/2018, 15:30
    PDFs, 𝛼ₛ and soft QCD

    The talk will cover measurements and QCD analyses of inclusive and differential
    top quark pairs and single top production, and of jets production, from ATLAS, CMS and LHCb.

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  79. Johannes Krause (TU Dresden)
    30/08/2018, 15:36
    Monte Carlo and Resummation

    We present a new algorithm to incorporate calculations with massive $b$-quarks, usually performed in the four flavour scheme, into a merged simulation obtained in the five flavour scheme. We apply this algorithm to $tt+\mathrm{jets}$ / $ttbb$ production, study the uncertainties of this newly developed method and compare our results to dedicated 4F/5F simulations.

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  80. 30/08/2018, 16:30
    Heavy Quarks

    Measurements of open charm and beauty production cross sections in deep inelastic $ep$ scattering at HERA from the H1 and ZEUS Collaborations are combined. Reduced cross sections are obtained in the kinematic range of negative four-momentum transfer squared of the photon $2.5$~GeV$^2\le Q^2 \le 2000$ GeV$^2$ and Bjorken scaling variable $3 \cdot 10^{-5} \le x_{\rm Bj} \le 5 \cdot 10^{-2}$. The...

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  81. Das Goutam (DESY Hamburg)
    30/08/2018, 16:30
    Monte Carlo and Resummation

    We study the transverse momentum spectrum for Drell-Yan production including the bottom mass effect. The pt-distribution of DY or Z boson is very important observable at the LHC, particularly to the ratio of W boson and Z boson spectrum to precisely measure of the W boson mass. The presence of an extra mass scale namely the bottom mass along with the hard scale and the pt-scale makes it very...

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  82. Prof. Gunnar Bali (Universität Regensburg)
    30/08/2018, 16:30
    PDFs, 𝛼ₛ and soft QCD

    Mellin moments of PDFs are calculable as expectation values of local operators within external states, using Lattice QCD. With sufficiently small statistical and systematic uncertainties, these provide information that will be complementary to parametrizations obtained from global fits to experimental data. I will present such lattice results.

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  83. Tobias Neumann (Illinois Tech / Fermi National Accelerator Laboratory)
    30/08/2018, 16:30
    Perturbative QCD, Jets and Substructure

    We present our calculation of next-to-leading order QCD effects in single top production for a precision determination of the Wtb coupling. The calculation is performed analytically with an off-shell top quark and includes relevant operators from the Standard Model Effective Field Theory (SMEFT) that modify the Wtb coupling also at next-to-leading order in QCD. We discuss the phenomenological...

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  84. Matthew DeAngelis
    30/08/2018, 16:52
    Monte Carlo and Resummation
  85. Zahari Dimitrov Kassabov Zaharieva (University of Cambridge (GB))
    30/08/2018, 17:00
    PDFs, 𝛼ₛ and soft QCD

    I present the recent determination of αs performed by the NNPDF collaboration. I particularly discuss the novel methodology adopted in the fit, as well as the breakdown of the uncertainties.

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  86. Peter Marquard (DESY)
    30/08/2018, 17:00
    Perturbative QCD, Jets and Substructure

    We present an overview of the current status of calculations for the QCD renormalization constants.

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  87. Dr Narayan Rana (DESY)
    30/08/2018, 17:00
    Heavy Quarks

    We present color planar and complete light quark QCD contributions to the three loop heavy quark form factors in the case of vector, axialvector, scalar and pseudoscalar currents. We evaluate the master integrals applying a new method based on differential equations for general bases, which is applicable for all first order factorizing systems. The analytic results are expressed in terms of...

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  88. Rudi Rahn (University of Bern)
    30/08/2018, 17:14
    Monte Carlo and Resummation

    Perturbative calculations for many collider observables suffer from large logarithmic corrections associated with soft emissions or radiation collinear to beam or jet directions. Resummation using SCET techniques is based on factorisation theorems, and requires the calculation of jet, soft and beam functions to some perturbative accuracy. This task has up to now mainly been achieved...

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  89. Bianca Scavino (Uni Mainz)
    30/08/2018, 17:30
    Heavy Quarks

    The Belle II experiment, now operating at the KEK laboratory in Japan, is a substantial upgrade of both the Belle detector and the KEKB $e^+ e^-$accelerator. It aims to collect 50 times more data than existing B-Factory samples. Belle II is uniquely capable to study the so-called "XYZ" particles: heavy exotic hadrons consisting of more than three quarks. First discovered by Belle, these now...

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  90. Dr Tie-Jiun Hou (Xinjiang University)
    30/08/2018, 17:30
    PDFs, 𝛼ₛ and soft QCD

    We will talk about the recent progress in the CTEQ-TEA global analysis.

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  91. Dr Dingyu Shao (CERN)
    30/08/2018, 17:36
    Monte Carlo and Resummation

    Starting from a factorization theorem in effective field theory, we derive a parton-shower equation for the resummation of non-global logarithms. We have implemented this shower and interfaced it with a tree-level event generator to obtain an automated framework to resum the leading logarithm of non-global observables in the large-Nc limit. Using this setup, we compute gap fractions for dijet...

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  92. Matteo Cacciari (LPTHE Jussieu), Satoshi Hasegawa (Fermi National Accelerator Lab. (US))
    31/08/2018, 09:00
  93. Luca Rottoli (University of Oxford)
    31/08/2018, 10:15
  94. Silvan Kuttimalai (SLAC)
    31/08/2018, 11:30
  95. Arantxa Ruiz Martinez (Univ. of Valencia and CSIC (ES))
    31/08/2018, 12:15
  96. 31/08/2018, 13:00
  97. ATLAS Collaboration
    Heavy Quarks

    Heavy quark spectroscopy and exotic states are studied with the ATLAS detector, mainly through final states containing muon pairs from J/psi decays. This talk will summarise recent results from ATLAS, including production of quarkonium and heavy flavour, searches for exotic states and measurements of decay properties in open beauty production.

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  98. Katharina Mueller (Universitaet Zuerich (CH))
    Heavy Quarks

    Measurements of CP violation are a core part of the LHCb physics
    programme and provide sensitivity to angles of the CKM matrix as well as
    probing our understanding of the differences between matter and
    antimatter. A summary of recent LHCb results are presented, including
    the time-dependent B0->Dpi analysis which profits from the largest
    flavour tagged sample analysed by LHCb, the world's first...

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  99. ATLAS Collaboration
    Monte Carlo and Resummation

    The total pp cross section is a fundamental observable at the LHC. It can be derived  from the measurement of the elastic cross section, using the optical theorem. Measurements of the elastic proton-proton cross section were performed at a center-of-mass energy of 8 TeV at various settings of the beam optics using the ALFA detector.
    The ALFA detector is also used to tag forward protons in...

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  100. CMS Collaboration
    Perturbative QCD, Jets and Substructure

    This talk describes the measurement of the jets mass and other jet substructure studies at CMS

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  101. Jian Wang
    Perturbative QCD, Jets and Substructure

    We calculate the N-jettiness soft function for tW production up to next-to-next-to-leading order in QCD, which is an important ingredient of the N-jettiness subtraction method for predicting the differential cross sections of massive coloured particle productions. We also compare the results with the predictions from renormalization group equations controlled by the soft anomalous dimension.

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  102. CMS Collaboration
    PDFs, 𝛼ₛ and soft QCD

    The associated production of vector bosons, W or Z, and jets originating from heavy-flavour quarks (HF) provide tests of pertubative QCD predictions and to the modelling of HF production. These measurements are sensitive to the heavy quark parton content of the proton and are input to PDF analyses. This talk should cover the recent V+ HF measurement done by the CMS detector.

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  103. Luca Rottoli (University of Oxford)
  104. Dr Hluf Negash (Samara University)
    Heavy Quarks

    In this study, we calculate the mass spectrum, weak decay constants, two photon decay widths, and two gluon decay widths of ground (1S), and radially excited (2S, 3S, 4S) states of pseudoscalar charmoniuum and bottomonium such as η_cand η_b, as well as the mass spectrum, leptonic decay constants and radiative decay widths of ground state (1S) and excited (2S, 1D, 3S, 2D, 4S,3D, 5S, 5D) states...

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  105. CMS Collaboration
    Heavy Quarks

    We present a search for the standard model Higgs boson decaying into b quarks and produced in association with a pair of top quarks decaying in the all-jet final state. This search is performed on 35.9 fb-1 of 13-TeV proton-proton collisions collected by the CMS experiment at the LHC. To separate the tt̄H signal from the irreducible tt̄ + bb̄ background, this analysis takes advantage of a...

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  106. CMS Collaboration
    Monte Carlo and Resummation

    Latest results from Underlying event measurements from ATLAS and CMS are presented.

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