26–30 Oct 2020
Europe/Rome timezone
There is a live webcast for this event.

Contribution List

138 out of 138 displayed
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  1. Paolo Meridiani (Sapienza Universita e INFN, Roma I (IT))
    26/10/2020, 12:30
  2. Anthony Morley (CERN)
    26/10/2020, 13:00
  3. Dr Pietro Vischia (Universite Catholique de Louvain (UCL) (BE))
    26/10/2020, 13:30
  4. Daniel De Florian (Laboratorio de Fisica Teorica Departamento de Fisica)
    26/10/2020, 14:20
  5. Valerio Dao (CERN)
    26/10/2020, 14:50
  6. Merijn Van De Klundert (Deutsches Elektronen-Synchrotron (DE))
    26/10/2020, 15:20
  7. Andrea Carlo Marini (Massachusetts Inst. of Technology (US))
    26/10/2020, 16:10
  8. Dr Luca Mastrolorenzo (Rheinisch Westfaelische Tech. Hoch. (DE))
    26/10/2020, 16:40
  9. Jim Olsen (Princeton University (US))
    26/10/2020, 17:30
  10. Hitoshi Murayama (University of California Berkeley (US))
    26/10/2020, 18:00
  11. Elisa Fontanesi (Universita e INFN, Bologna (IT))
    27/10/2020, 12:30
    Precision Session
  12. Fady Adibsamy Bishara (DESY)
    27/10/2020, 12:30
    Yukawa Session
  13. Lata Panwar (Indian Institute of science (IN))
    27/10/2020, 12:30
    HH Session
  14. Reina Coromoto Camacho Toro (Centre National de la Recherche Scientifique (FR))
    27/10/2020, 12:50
    Yukawa Session
  15. Jonas Lindert (University of Sussex)
    27/10/2020, 12:50
    Precision Session
  16. Bowen Zhang (Nanjing University (CN))
    27/10/2020, 12:50
    HH Session
  17. Bjorn Burkle (Brown University (US))
    27/10/2020, 13:10
    Yukawa Session
  18. Eleni Vryonidou
    27/10/2020, 13:10
    Precision Session
  19. Dr Rahool Kumar Barman (Indian Association for the Cultivation of Sciences, Kolkata, India)
    27/10/2020, 13:10
    HH Session
  20. Milada Muhlleitner (KIT - Karlsruhe Institute of Technology (DE)), Milada Muhlleitner
    27/10/2020, 13:30
  21. Tanjona Radonirina Rabemananjara (INFN - National Institute for Nuclear Physics), Tanjona Radonirina Rabemananjara (CERN)
    27/10/2020, 13:30
  22. Davide Zuliani (Universita e INFN, Padova (IT))
    27/10/2020, 13:30
    Yukawa Session
  23. Matthew Basso (University of Toronto (CA))
    27/10/2020, 14:20
    Precision Session
  24. Joachim Brod (University of Cincinnati)
    27/10/2020, 14:20
    Yukawa Session
  25. Jason Robert Veatch (Georg August Universitaet Goettingen (DE))
    27/10/2020, 14:20
    HH Session
  26. Dimitris Fassouliotis (National and Kapodistrian University of Athens (GR))
    27/10/2020, 14:40
    Precision Session
  27. Soumya Mukherjee (Tata Inst. of Fundamental Research (IN))
    27/10/2020, 14:40
    HH Session
  28. Andrew David Loeliger (University of Wisconsin Madison (US))
    27/10/2020, 14:40
    Yukawa Session
  29. Arnd Behring (Karlsruhe Institute of Technology (KIT))
    27/10/2020, 15:00
    Precision Session
  30. Yehonatan Viernik (Weizmann)
    27/10/2020, 15:00
    Yukawa Session
  31. Seraina Glaus (E), Seraina Glaus (KIT)
    27/10/2020, 15:00
    HH Session
  32. Miha Muskinja (Lawrence Berkeley National Lab. (US))
    27/10/2020, 15:20
    Yukawa Session
  33. Shireen Gangal
    27/10/2020, 15:20
    Precision Session
  34. José Francisco Zurita (KIT)
    27/10/2020, 15:20
    HH Session
  35. Jan Oliver Rieger (Hamburg University (DE))
    27/10/2020, 15:35
    Yukawa Session
  36. 27/10/2020, 15:40
  37. 27/10/2020, 15:40
  38. 27/10/2020, 15:50
  39. Bianca Monica Ciungu (University of Toronto (CA))
    27/10/2020, 16:10
    YSF
  40. Benjamin Paul Jaeger (Simon Fraser University (CA))
    27/10/2020, 16:15
    YSF
  41. Wai Yuen Chan (University of Liverpool (GB)), Wai Yuen Chan (University of Liverpool)
    27/10/2020, 16:20
    YSF
  42. Jay Chan (University of Wisconsin Madison (US))
    27/10/2020, 16:25
    YSF
  43. Zhijun Liang (Chinese Academy of Sciences (CN))
    27/10/2020, 16:40
  44. Valeria Botta (Deutsches Elektronen-Synchrotron (DE))
    27/10/2020, 17:10
  45. Simone Amoroso (Deutsches Elektronen-Synchrotron (DE))
    27/10/2020, 17:40
  46. Davide Pietro Mungo (Università degli Studi e INFN Milano (IT))
    28/10/2020, 12:30
    Precision Session
  47. Liron Barak (Tel Aviv University)
    28/10/2020, 12:30
    BSM Session
  48. Brian Moser (Nikhef National institute for subatomic physics (NL))
    28/10/2020, 12:30
    EFT Session
  49. Doyeong Kim (KANSAS STATE UNIVERSITY)
    28/10/2020, 12:50
    Precision Session
  50. Dominik Duda (Max-Planck-Institut fur Physik (DE))
    28/10/2020, 12:52
    BSM Session
  51. Ashish Sharma (Indian Institute of Technology Madras (IN))
    28/10/2020, 13:00
    EFT Session
  52. Dr Alexander Karlberg (University of Oxford)
    28/10/2020, 13:10
    Precision Session
  53. Zhen Liu (U of Maryland)
    28/10/2020, 13:14
    BSM Session
  54. Filippo Errico (University of Florida (US))
    28/10/2020, 13:30
    Precision Session
  55. Michael Robert Trott (University of Copenhagen (DK))
    28/10/2020, 13:30
    EFT Session
  56. 28/10/2020, 13:36
    BSM Session
  57. 28/10/2020, 13:50
  58. Danyer Perez Adan (Deutsches Elektronen-Synchrotron (DE))
    28/10/2020, 14:20
    BSM Session
  59. Alexandre Salas-Bernárdez (Universidad Complutense de Madrid)
    28/10/2020, 14:20
    EFT Session
  60. Irene Dutta (California Institute of Technology (US))
    28/10/2020, 14:20
    Precision Session
  61. Parisa Gregg
    28/10/2020, 14:40
    EFT Session
  62. Dr Lucian Harland-Lang (University of Oxford)
    28/10/2020, 14:40
    Precision Session
  63. Dr Alexandros Attikis (University of Cyprus (CY))
    28/10/2020, 14:42
    BSM Session
  64. Xing Wang (UC San Diego)
    28/10/2020, 15:00
    Precision Session
  65. Samuel Homiller (Harvard)
    28/10/2020, 15:00
    EFT Session
  66. Da Liu (UC, Davis)
    28/10/2020, 15:04
    BSM Session
  67. Ulascan Sarica (Univ. of California Santa Barbara (US))
    28/10/2020, 15:20
    EFT Session
  68. Gauthier Durieux (CERN)
    28/10/2020, 15:20
    Precision Session
  69. Brian Shuve (Harvey Mudd College)
    28/10/2020, 15:26
    BSM Session
  70. 28/10/2020, 15:40
    EFT Session
  71. Nathaniel Craig (UC Santa Barbara)
    28/10/2020, 16:00

    25' (5' discussion)

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  72. Verena Ingrid Martinez Outschoorn (University of Massachusetts (US))
    28/10/2020, 16:30
  73. Jessie Shelton (Yale University)
    28/10/2020, 17:00
  74. Benedikt Maier (Massachusetts Inst. of Technology (US))
    28/10/2020, 17:30
  75. Luciano Maiani (Unknown), Luciano Maiani (Sapienza Universita e INFN, Roma I (IT))
    28/10/2020, 18:00
  76. Konstantinos Nikolopoulos (University of Birmingham (GB))
    29/10/2020, 12:30
    HH Session
  77. Ian Allan Connelly (University of Glasgow (GB))
    29/10/2020, 12:30
    Yukawa Session
  78. Arianna Rocchetti, Arianna Rocchetti (University of Freiburg)
    29/10/2020, 12:30
    BSM Session
  79. Michele Selvaggi (CERN)
    29/10/2020, 12:50
    HH Session
  80. Clara Ramon Alvarez (Universidad de Oviedo (ES))
    29/10/2020, 12:50
    Yukawa Session
  81. Samuel Ross Meehan (CERN)
    29/10/2020, 12:52
    BSM Session
  82. Shankha Banerjee (CERN), Dr Shankha Banerjee (Institute for Particle Physics Phenomenology, Durham University, UK)
    29/10/2020, 13:10
    HH Session
  83. Matthias Schlaffer (University of Chicago)
    29/10/2020, 13:10
    Yukawa Session
  84. Prasanna Kumar Siddireddy (University of Notre Dame (US))
    29/10/2020, 13:14
    BSM Session
  85. Andreas Crivellin (Universitaet Zuerich (CH))
    29/10/2020, 13:30
    Yukawa Session
  86. Barbara Mele (Sapienza Universita e INFN, Roma I (IT))
    29/10/2020, 13:30
    HH Session
  87. Samuel Homiller (Harvard)
    29/10/2020, 13:36
    BSM Session
  88. Elizabeth Brost (Brookhaven National Laboratory (US))
    29/10/2020, 14:20
  89. Agni Bethani (Universite Catholique de Louvain (UCL) (BE))
    29/10/2020, 14:50
  90. Stephen Philip Jones (CERN)
    29/10/2020, 15:20
  91. Mohammadhassan Hassanshahi (Imperial College (GB))
    29/10/2020, 16:00
    YSF
  92. Krunal Bipin Gedia (ETH Zurich (CH))
    29/10/2020, 16:05
    YSF
  93. Dmitry Kondratyev (Purdue University (US))
    29/10/2020, 16:10
    YSF
  94. Xunwu Zuo (University of Florida (US))
    29/10/2020, 16:15
    YSF
  95. Francesco Riva (Universite de Geneve (CH))
    29/10/2020, 16:30
  96. Saskia Falke (CERN)
    29/10/2020, 17:00
  97. Oscar Jose Pinto Eboli (Federal University of of Rio de Janeiro (BR))
    29/10/2020, 17:30
  98. Kyle Stuart Cranmer (New York University (US))
    30/10/2020, 12:30
  99. Felix Kling (SLAC)
    30/10/2020, 13:00
  100. Stefan Hoeche (Fermilab)
    30/10/2020, 13:30
  101. Caterina Vernieri (SLAC National Accelerator Laboratory (US))
    30/10/2020, 14:00
  102. Laura Reina (Florida State University (US))
    30/10/2020, 15:00
  103. Pierre Savard (University of Toronto (CA))
    30/10/2020, 15:30
  104. Christophe Grojean (DESY (Hamburg) and Humboldt University (Berlin))
    30/10/2020, 16:00
  105. Tilman Plehn
    30/10/2020, 16:30
  106. Arnd Behring (Karlsruhe Institute of Technology (KIT))
    Precision Session

    We present a computation of next-to-next-to-leading-order (NNLO) QCD corrections to the production of a Higgs boson in association with a $W$ boson at the LHC followed by the decay of the Higgs boson to a $b\bar{b}$ pair. At variance with previous NNLO QCD studies of the same process, we treat $b$ quarks as massive. An important advantage of working with massive b quarks is that it makes the...

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  107. Arnd Behring (Karlsruhe Institute of Technology (KIT))
    Precision Session
  108. Tanjona Radonirina Rabemananjara (INFN - National Institute for Nuclear Physics)
    Precision Session

    We present new phenomenological studies of the impact of a recently suggested formalism that simultaneously resums logarithmic contributions that are enhanced at small $p_T$ and large $x$. This formalism relies on the combination of a so-called threshold-improved transverse momentum and threshold resummation which allows for a systematic improvement of the transverse momentum resummation that...

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  109. Parisa Gregg
    EFT Session

    As the search for physics beyond the Standard Model (BSM) continues, the Standard Model Effective Field Theory (SMEFT) has become a useful tool to constrain deviations from the SM in a model-independent way. In this talk we will consider the associated production of a Higgs boson and a photon in weak boson fusion (WBF), with the Higgs boson decaying to a pair of bottom quarks. I will present a...

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  110. Parisa Gregg
    EFT Session
  111. Alexandre Salas-Bernárdez (Universidad Complutense de Madrid)
    EFT Session

    Effective Field Theories (EFTs) constructed, in the spirit of Chiral Perturbation Theory (ChPT), as derivative expansions in powers of momentum, are a controllable approximation to strong dynamics as long as the energy of the interacting particles remains small. However, deviations quickly build up due to the energy--polynomial expansion not respecting unitarity. This limits their predictive...

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  112. Yukawa Session

    Recently, both ATLAS and CMS measured the decay h→μ+μ−, finding a signal strength with respect to the Standard Model (SM) expectation of 1.2±0.6 and 1.19+0.41+0.17−0.39−0.16, respectively. This measurement is particularly interesting in the context of the existing hints for lepton flavor universality violation (LFUV), since their new physics explanations could be tested in this decay mode....

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  113. EFT Session
  114. Xing Wang (University of Pittsburgh)
    Precision Session

    We estimate the expected precision at a multi-TeV muon collider for measuring the Higgs boson couplings with electroweak gauge bosons, $HVV$ and $HHVV\ (V=W^\pm,Z)$, as well as the trilinear Higgs self-coupling $HHH$. At very high energies both single and double Higgs productions rely on the vector-boson fusion (VBF) topology. The outgoing remnant particles have a strong tendency to stay in...

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  115. Precision Session
  116. EFT Session

    We develop the geometric formulation of the Standard Model Effective Field Theory (SMEFT). Using this approach we derive all-orders results in the vev expansion
    relevant for studies of electroweak precision and Higgs data, as reported in
    https://arxiv.org/pdf/2001.01453.pdf. Then using this formalism we report the first exact formalism to sub-leading order in the vev expansion as applied to...

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  117. Oscar Jose Pinto Eboli (Federal University of of Rio de Janeiro (BR))
  118. EFT Session
  119. Precision Session
  120. LHCb Collaboration
    Yukawa Session

    Thanks to the excellent vertex reconstruction system, the LHCb detector has demonstrated its capabilities in the identification of b- and c-jets.
    The LHCb upgrades could be used to measure the H->bb production in a region complementary to ATLAS and CMS, and to search for the H->cc decay.
    In this talk the jet heavy flavour tagging algorithm used at LHCb is reviewed, and measurements with b-...

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  121. Precision Session
  122. EFT Session

    The JHU generator framework includes an event generator of anomalous HVV and Hff interactions of the Higgs boson in production and decay and a MELA library for matrix element analysis. This framework allows constraints on dimension-six operators of an effective field theory from a joint analysis of on-shell and off-shell production of the Higgs boson and of triple and quartic gauge boson...

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  123. Precision Session
  124. Francesco Riva (Universite de Geneve (CH))
  125. Dr Samuel Homiller (Harvard)
    EFT Session

    The Standard Model Effective Field Theory (SMEFT) provides a consistent framework for comparing precision measurements at the LHC to the Standard Model (SM). The observation of statistically significant non-zero SMEFT coefficients would correspond to physics beyond the SM (BSM) of some sort. A more difficult question to answer is what, if any, detailed information about the nature of the...

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  126. Stephen Philip Jones (CERN)