24–26 May 2021
University of Pittsburgh
US/Eastern timezone

Session

Higgs IV

26 May 2021, 16:30

Conveners

Higgs IV

  • Dorival Goncalves (Oklahoma State University)

Presentation materials

  1. Victor Baules (University of Alabama, The)
    26/05/2021, 16:30
    Higgs

    We consider a classically conformal $U(1)$ extension of the Standard Model (SM). The $U(1)$ symmetry is radiatively broken by the Coleman-Weinberg mechanism, after which the $U(1)$ Higgs field $\phi$ drives electroweak symmetry breaking through a mixed quartic coupling with the SM Higgs doublet with coupling constant $\lambda_{mix}$. We calculate the Higgs triple couplings in this system and...

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  2. Dr Da Liu (UC, Davis)
    26/05/2021, 16:45

    Recently an on-shell formalism of scattering amplitudes for all masses and spins have been developed by Nima, Tzu-Chen and Yu-tin. In particular, Higgs mechanism can be understood as IR unification of different UV massless helicity amplitudes. This is complementary to the classic results by Cornwall et al, who have proved that the only consistent UV theory of interacting massive scalar,...

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  3. Mr Pedro Bittar (University of São Paulo)
    26/05/2021, 17:00
    Higgs

    The presence of heavy new physics generally alters the Standard Model (SM) Higgs couplings predictions. In many models, momentum effects are assumed to decouple as the heavy states are integrated out. However, these effects can be important in situations of significant off-shellness at collider experiments. In this talk, I will discuss the momentum dependence of different beyond the SM...

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  4. SHILPA JANGID (IIT HYDERABAD)
    26/05/2021, 17:15
    Higgs

    The Standard Model (SM) explaining the framework of elementary particles seems to be completed
    by the discovery of the SM-like Higgs boson with a mass of about 125 GeV at the Large Hadron
    Collider(LHC) in 2012. Despite this success, there are enough experimental evidences, ranging
    from observed dark matter (DM) relic density and matter-antimatter asymmetry in the universe
    to non-zero...

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  5. Han Qin (University of Pittsburgh)
    26/05/2021, 17:30
    Higgs

    We explore the new physics reach for the off-shell Higgs boson measurement in the ${pp \to H^* \rightarrow Z(\ell^{+}\ell^{-})Z(\nu\bar{\nu})}$ channel at the high-luminosity LHC. The new physics sensitivity is parametrized in terms of the Higgs boson width, effective field theory framework, and a non-local Higgs-top coupling form factor. Adopting Machine-learning techniques, we demonstrate...

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  6. Roshan Mammen Abraham (Oklahoma State University)
    26/05/2021, 17:45
    BSM

    The top-quark Yukawa coupling $y_t$ is the strongest interaction of the Higgs boson in the Standard Model (SM) with $y_t \sim 1$. Due to its magnitude, it plays a central role in Higgs phenomenology in the SM and would be most sensitive to physics beyond the Standard Model. The top Yukawa can be directly measured at the LHC via top pair production in association with a Higgs boson...

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  7. Mudit Rai (University of Pittsburgh)
    26/05/2021, 18:00

    "Singlet scalar mediators have a wide phenomenological application and a variety of SM extensions have been based on them. In this work, we build upon the story of flavor-specific scalars, where the scalar dominantly couples to one specific SM fermion mass eigenstate. This hypothesis meshes well with absence of new flavor changing neutral currents at tree level. Earlier works were based on an...

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  8. Terrance Figy (Wichita State University)
    26/05/2021, 18:15
    Higgs

    In this talk I will present results of the simulation of electroweak Higgs boson production at the CERN LHC using the Herwig 7 general purpose event generator using one-loop matrix elements via the interface to HJets. The main result will be the simulation of next-to-leading order merging of Higgs boson plus 2 and 3 jets with a dipole parton shower. Additionally, I will comment on...

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  9. Chandiprasad Kar (National Institute of Science Education and Research (IN))
    26/05/2021, 18:30

    The most recent result achieved by the CMS experiment in the field of Heavy Flavour and Quarkonia Physics will be presented and discussed with emphasis to the brand new measurements and observations.

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