7โ€“12 Feb 2022
Institute of Physics, Bhubaneswar
Asia/Kolkata timezone

Contribution List

46 out of 46 displayed
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  1. 07/02/2022, 14:00
  2. Clifford Peter Burgess (McMaster University (CA))
    07/02/2022, 14:15
  3. Luca Silvestrini (CERN and INFN, Rome)
    07/02/2022, 16:00
  4. Eleni Vryonidou (University of Manchester (GB))
    07/02/2022, 17:30
  5. Kaladi Babu (Oklahoma State University)
    08/02/2022, 09:30
  6. Dr Sudip Jana
    08/02/2022, 11:00
  7. Clifford Peter Burgess (McMaster University (CA))
    08/02/2022, 14:00
  8. Martin Hirsch
    08/02/2022, 16:00
  9. Michael Robert Trott (University of Copenhagen (DK))
    09/02/2022, 09:30
  10. Subhaditya Bhattacharya
    09/02/2022, 11:30
  11. John Ellis (Kings College London)
    09/02/2022, 16:00
  12. Gino Isidori (University of Zurich (CH))
    09/02/2022, 17:30
  13. Sally Dawson (BNL)
    09/02/2022, 19:00
  14. Michael Robert Trott (University of Copenhagen (DK))
    10/02/2022, 09:30
  15. Joydeep Chakrabortty (IIT Kanpur)
    10/02/2022, 11:30
  16. Rajeev N
    10/02/2022, 14:30
  17. ROJALIN PADHAN (Institute of Physics, Bhubaneswar)
    10/02/2022, 14:50
  18. Rahool Kumar Barman
    10/02/2022, 15:10
  19. Tisa Biswas (University of Calcutta)
    10/02/2022, 15:30
  20. Bibhabasu De (IOP Bhubaneswar)
    10/02/2022, 15:50
  21. Soumya Mukherjee (Tata Inst. of Fundamental Research (IN))
    10/02/2022, 16:30
  22. Upalaparna Banerjee
    10/02/2022, 16:50
  23. shakeel ur rahaman
    10/02/2022, 17:10
  24. Suraj Prakash
    10/02/2022, 17:30
  25. Roshan Mammen Abraham (Oklahoma State University)
    10/02/2022, 17:50
  26. Tim M.P. Tait (University of California, Irvine)
    11/02/2022, 09:30
  27. Michael Robert Trott (University of Copenhagen (DK))
    11/02/2022, 10:30
  28. Ambresh Shivaji (IISER Mohali)
    11/02/2022, 12:00
  29. Adam Falkowski (LPT Orsay)
    11/02/2022, 14:00
  30. Jiang-Hao Yu
    11/02/2022, 16:00
  31. Andrei Gritsan (Johns Hopkins University (US))
    11/02/2022, 19:00
  32. Adam Falkowski (LPT Orsay)
    12/02/2022, 14:00
  33. John Ellis (Kings College London)
    12/02/2022, 16:00
  34. Mr shakeel ur rahaman
    Contributory talks

    The success of the Standard Model (SM) and the lack of direct evidence of any beyond Standard Model (BSM) particles impels us to look for indirect shreds of evidence. The effective field theory framework is just the right tool for that. We can treat the SM as an effective theory by adding higher dimensional terms to its Lagrangian and trying to capture the footprint of the more complete UV...

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  35. Mr Bibhabasu De (ICFAI University Tripura)
    Contributory talks

    Extensive searches to probe the particle nature of dark matter (DM) have been going on for some decades now but, so far, no conclusive evidence has been found. Among various options, the Weakly Interacting Massive Particles (WIMP) remains one of the prime
    possibilities as candidates for DM near the TeV scale. Taking a phenomenological view, such null results may be explained for a generic...

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  36. Rajeev N
    Contributory talks

    The long persistent discrepancies in $b\,\to\,s\, \ell\, \ell$ quark level transitions continue to be the
    ideal platform for an indirect search of new physics that lies beyond the standard model. The recent updated measurements of $R_K$, $\mathcal{B}(B_s\, \to\, \phi\, \mu^+\,\mu^-)$
    and $\mathcal{B}(B_s\, \to\, \mu^+\,\mu^-)$ from LHCb persistently deviate from the standard model...

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  37. Rahool Kumar Barman (Oklahoma State University)
    Contributory talks

    We explore the projected sensitivity for SMEFT coefficients $\mathcal{C}_{tZ}$ and $\mathcal{C}_{tW}$ via single top $ pp \to tZj$ and top pair associated production $pp \to t\bar{t}Z$ channels with machine learning techniques, at the high luminosity LHC. Implications from new physics modifications in relevant background processes are also included. We identify the subset of observables that...

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  38. Roshan Mammen Abraham (Oklahoma State University)
    Contributory talks

    The top-quark Yukawa coupling, $y_t$ is the strongest interaction of the Higgs
    boson in the Standard Model (SM) with $y_t$โˆผ1. 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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  39. Mr Suraj Prakash
    Contributory talks

    The Standard Model Effective Field Theory (SMEFT) is an established theoretical framework that parametrizes the impact of UV models on low-energy observables. Such parametrization is achieved by studying the interactions of SM fields encapsulated within higher mass dimensional ($\geq$ 5) operators. Through judicious employment of the EFT toolkit, SMEFT has become a source of new predictions as...

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  40. Soumya Mukherjee (Tata Inst. of Fundamental Research (IN))
    Contributory talks

    The trilinear self-coupling (ฮป) of Higgs can directly be accessed at the LHC by inclusive production of Higgs boson pair. A search for the non-resonant Higgs pair production via gluon-gluon fusion and as well as Vector Boson Fusion processes has been performed recently by CMS collaboration in various final state with the complete LHC Run-2 proton-proton collision data at center of mass energy...

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  41. Clifford Burgess (High Energy Physics Group - McGill University), Clifford Peter Burgess (McMaster University (CA))
  42. Ms Upalaparna Banerjee (IIT Kanpur)
    Contributory talks

    The spectrum of the new physics beyond the Standard Model is very likely to be non-degenerate with few light non-SM particles residing close to the electroweak scale. The effect of the more complete theory then can be captured through an effective extension of the BSM scenario treating the new non-SM particles on the same footing along with the SM ones. To perform a detailed phenomenological...

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  43. Luca Silvestrini, Luca Silvestrini (CERN and INFN, Rome)
  44. Eleni Vryonidou (University of Manchester (GB))
  45. Ms ROJALIN PADHAN (Institute of Physics, Bhubaneswar)
    Contributory talks

    We consider an effective field theory framework with three standard model (SM) gauge singlet right handed neutrinos, and an additional SM gauge singlet scalar field. The framework successfully generates eV masses of the light neutrinos via seesaw mechanism, and accommodates a feebly interacting massive particle (FIMP) as dark matter candidate. Two of the gauge singlet neutrinos ...

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