4–8 Nov 2024
Uppsala University Main Building
Europe/Stockholm timezone

Session

Common session: precision & BSM 2 - sal IX

6 Nov 2024, 15:20
Uppsala University Main Building

Uppsala University Main Building

Biskopsgatan 3 75310 Uppsala Sweden

Conveners

Common session: precision & BSM 2 - sal IX

  • Stefano Manzoni (CERN)
  • Eleni Vryonidou (The University of Manchester (GB))
  • Stephen Philip Jones (University of Durham (GB))
  • Daniel Winterbottom (Imperial College (GB))
  • Rafael Coelho Lopes De Sa (University of Massachusetts (US))
  • Susan J Dittmer (Northwestern University (US))

Presentation materials

There are no materials yet.

  1. Mohammad Alminawi (University of Zurich (CH))
    06/11/2024, 15:20
    Precision Higgs measurements and calculations

    Geometric formulations of scalar EFTs formulate fields as coordinates on a field space manifold, which provides an alternative method of studying theories by relating physical quantities emerging from the two derivative term to geometric tensors which are invariant under field redefinitions.

    Fibre bundles provide us with the tools to extend the formalism to both describe the potential via...

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  2. Marco Menen (Leibniz Universität Hannover)
    06/11/2024, 15:40
    BSM Higgs physics

    The $\mathcal{CP}$ structure of the Higgs couplings is a fundamental property which has not yet been constrained with high precision. The Higgs-top quark coupling is of particular interest due to its size and accessibility at the LHC via top-associated Higgs production and gluon fusion. To improve the sensitivity to the CP property of this coupling, we propose an extension to the STXS...

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  3. Ya-Juan Zheng
    06/11/2024, 16:00
    BSM Higgs physics

    We study the single top plus Higgs production process at the LHC with a CP violating Yukawa coupling from a dimension-6 operator. The amplitude of the subprocess ub>dtH is obtained both in the Unitary (U) and Feynman-Diagram (FD) gauges. Energy and angular distributions of the cross section and CP violating asymmetries are understood clearly from the interference among the FD gauge amplitudes.

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