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Paolo Meridiani (Sapienza Universita e INFN, Roma I (IT))26/10/2020, 12:30
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Anthony Morley (CERN)26/10/2020, 13:00
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Dr Pietro Vischia (Universite Catholique de Louvain (UCL) (BE))26/10/2020, 13:30
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Daniel De Florian (Laboratorio de Fisica Teorica Departamento de Fisica)26/10/2020, 14:20
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Valerio Dao (CERN)26/10/2020, 14:50
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Merijn Van De Klundert (Deutsches Elektronen-Synchrotron (DE))26/10/2020, 15:20
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Andrea Carlo Marini (Massachusetts Inst. of Technology (US))26/10/2020, 16:10
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Dr Luca Mastrolorenzo (Rheinisch Westfaelische Tech. Hoch. (DE))26/10/2020, 16:40
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Jim Olsen (Princeton University (US))26/10/2020, 17:30
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Hitoshi Murayama (University of California Berkeley (US))26/10/2020, 18:00
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Elisa Fontanesi (Universita e INFN, Bologna (IT))27/10/2020, 12:30Precision Session
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Fady Adibsamy Bishara (DESY)27/10/2020, 12:30Yukawa Session
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Lata Panwar (Indian Institute of science (IN))27/10/2020, 12:30HH Session
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Reina Coromoto Camacho Toro (Centre National de la Recherche Scientifique (FR))27/10/2020, 12:50Yukawa Session
EXP (ATLAS+CMS)
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Jonas Lindert (University of Sussex)27/10/2020, 12:50Precision Session
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Bowen Zhang (Nanjing University (CN))27/10/2020, 12:50HH Session
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Bjorn Burkle (Brown University (US))27/10/2020, 13:10Yukawa Session
EXP (ATLAS+CMS)
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Eleni Vryonidou27/10/2020, 13:10Precision Session
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Dr Rahool Kumar Barman (Indian Association for the Cultivation of Sciences, Kolkata, India)27/10/2020, 13:10HH Session
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Milada Muhlleitner (KIT - Karlsruhe Institute of Technology (DE)), Milada Muhlleitner27/10/2020, 13:30
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Tanjona Radonirina Rabemananjara (INFN - National Institute for Nuclear Physics), Tanjona Radonirina Rabemananjara (CERN)27/10/2020, 13:30
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Davide Zuliani (Universita e INFN, Padova (IT))27/10/2020, 13:30Yukawa Session
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Matthew Basso (University of Toronto (CA))27/10/2020, 14:20Precision Session
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Joachim Brod (University of Cincinnati)27/10/2020, 14:20Yukawa Session
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Jason Robert Veatch (Georg August Universitaet Goettingen (DE))27/10/2020, 14:20HH Session
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Dimitris Fassouliotis (National and Kapodistrian University of Athens (GR))27/10/2020, 14:40Precision Session
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Soumya Mukherjee (Tata Inst. of Fundamental Research (IN))27/10/2020, 14:40HH Session
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Andrew David Loeliger (University of Wisconsin Madison (US))27/10/2020, 14:40Yukawa Session
EXP (ATLAS+CMS)
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Arnd Behring (Karlsruhe Institute of Technology (KIT))27/10/2020, 15:00Precision Session
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Yehonatan Viernik (Weizmann)27/10/2020, 15:00Yukawa Session
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Seraina Glaus (E), Seraina Glaus (KIT)27/10/2020, 15:00HH Session
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Miha Muskinja (Lawrence Berkeley National Lab. (US))27/10/2020, 15:20Yukawa Session
EXP (ATLAS)
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Shireen Gangal27/10/2020, 15:20Precision Session
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José Francisco Zurita (KIT)27/10/2020, 15:20HH Session
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Jan Oliver Rieger (Hamburg University (DE))27/10/2020, 15:35Yukawa Session
EXP (CMS)
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27/10/2020, 15:40
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27/10/2020, 15:40
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27/10/2020, 15:50
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Bianca Monica Ciungu (University of Toronto (CA))27/10/2020, 16:10
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Benjamin Paul Jaeger (Simon Fraser University (CA))27/10/2020, 16:15
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Wai Yuen Chan (University of Liverpool (GB)), Wai Yuen Chan (University of Liverpool)27/10/2020, 16:20
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Jay Chan (University of Wisconsin Madison (US))27/10/2020, 16:25
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Zhijun Liang (Chinese Academy of Sciences (CN))27/10/2020, 16:40
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Valeria Botta (Deutsches Elektronen-Synchrotron (DE))27/10/2020, 17:10
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Simone Amoroso (Deutsches Elektronen-Synchrotron (DE))27/10/2020, 17:40
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Davide Pietro Mungo (Università degli Studi e INFN Milano (IT))28/10/2020, 12:30Precision Session
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Liron Barak (Tel Aviv University)28/10/2020, 12:30BSM Session
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Brian Moser (Nikhef National institute for subatomic physics (NL))28/10/2020, 12:30EFT Session
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Doyeong Kim (KANSAS STATE UNIVERSITY)28/10/2020, 12:50Precision Session
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Dominik Duda (Max-Planck-Institut fur Physik (DE))28/10/2020, 12:52BSM Session
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Ashish Sharma (Indian Institute of Technology Madras (IN))28/10/2020, 13:00EFT Session
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Dr Alexander Karlberg (University of Oxford)28/10/2020, 13:10Precision Session
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Zhen Liu (U of Maryland)28/10/2020, 13:14BSM Session
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Filippo Errico (University of Florida (US))28/10/2020, 13:30Precision Session
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Michael Robert Trott (University of Copenhagen (DK))28/10/2020, 13:30EFT Session
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28/10/2020, 13:36BSM Session
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28/10/2020, 13:50
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Danyer Perez Adan (Deutsches Elektronen-Synchrotron (DE))28/10/2020, 14:20BSM Session
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Alexandre Salas-Bernárdez (Universidad Complutense de Madrid)28/10/2020, 14:20EFT Session
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Irene Dutta (California Institute of Technology (US))28/10/2020, 14:20Precision Session
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Parisa Gregg28/10/2020, 14:40EFT Session
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Dr Lucian Harland-Lang (University of Oxford)28/10/2020, 14:40Precision Session
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Dr Alexandros Attikis (University of Cyprus (CY))28/10/2020, 14:42BSM Session
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Xing Wang (UC San Diego)28/10/2020, 15:00Precision Session
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Samuel Homiller (Harvard)28/10/2020, 15:00EFT Session
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Da Liu (UC, Davis)28/10/2020, 15:04BSM Session
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Ulascan Sarica (Univ. of California Santa Barbara (US))28/10/2020, 15:20EFT Session
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Gauthier Durieux (CERN)28/10/2020, 15:20Precision Session
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Brian Shuve (Harvey Mudd College)28/10/2020, 15:26BSM Session
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28/10/2020, 15:40EFT Session
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Nathaniel Craig (UC Santa Barbara)28/10/2020, 16:00
25' (5' discussion)
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Verena Ingrid Martinez Outschoorn (University of Massachusetts (US))28/10/2020, 16:30
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Jessie Shelton (Yale University)28/10/2020, 17:00
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Benedikt Maier (Massachusetts Inst. of Technology (US))28/10/2020, 17:30
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Luciano Maiani (Unknown), Luciano Maiani (Sapienza Universita e INFN, Roma I (IT))28/10/2020, 18:00
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Konstantinos Nikolopoulos (University of Birmingham (GB))29/10/2020, 12:30HH Session
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Ian Allan Connelly (University of Glasgow (GB))29/10/2020, 12:30Yukawa Session
EXP (ATLAS+CMS)
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Arianna Rocchetti, Arianna Rocchetti (University of Freiburg)29/10/2020, 12:30BSM Session
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Michele Selvaggi (CERN)29/10/2020, 12:50HH Session
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Clara Ramon Alvarez (Universidad de Oviedo (ES))29/10/2020, 12:50Yukawa Session
EXP (ATLAS+CMS)
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Samuel Ross Meehan (CERN)29/10/2020, 12:52BSM Session
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Shankha Banerjee (CERN), Dr Shankha Banerjee (Institute for Particle Physics Phenomenology, Durham University, UK)29/10/2020, 13:10HH Session
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Matthias Schlaffer (University of Chicago)29/10/2020, 13:10Yukawa Session
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Prasanna Kumar Siddireddy (University of Notre Dame (US))29/10/2020, 13:14BSM Session
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Andreas Crivellin (Universitaet Zuerich (CH))29/10/2020, 13:30Yukawa Session
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Barbara Mele (Sapienza Universita e INFN, Roma I (IT))29/10/2020, 13:30HH Session
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Samuel Homiller (Harvard)29/10/2020, 13:36BSM Session
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Elizabeth Brost (Brookhaven National Laboratory (US))29/10/2020, 14:20
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Agni Bethani (Universite Catholique de Louvain (UCL) (BE))29/10/2020, 14:50
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Stephen Philip Jones (CERN)29/10/2020, 15:20
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Mohammadhassan Hassanshahi (Imperial College (GB))29/10/2020, 16:00
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Krunal Bipin Gedia (ETH Zurich (CH))29/10/2020, 16:05
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Dmitry Kondratyev (Purdue University (US))29/10/2020, 16:10
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Xunwu Zuo (University of Florida (US))29/10/2020, 16:15
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Francesco Riva (Universite de Geneve (CH))29/10/2020, 16:30
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Saskia Falke (CERN)29/10/2020, 17:00
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Oscar Jose Pinto Eboli (Federal University of of Rio de Janeiro (BR))29/10/2020, 17:30
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Kyle Stuart Cranmer (New York University (US))30/10/2020, 12:30
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Felix Kling (SLAC)30/10/2020, 13:00
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Stefan Hoeche (Fermilab)30/10/2020, 13:30
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Caterina Vernieri (SLAC National Accelerator Laboratory (US))30/10/2020, 14:00
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Laura Reina (Florida State University (US))30/10/2020, 15:00
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Pierre Savard (University of Toronto (CA))30/10/2020, 15:30
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Christophe Grojean (DESY (Hamburg) and Humboldt University (Berlin))30/10/2020, 16:00
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Tilman Plehn30/10/2020, 16:30
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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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Arnd Behring (Karlsruhe Institute of Technology (KIT))Precision Session
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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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Parisa GreggEFT 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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Parisa GreggEFT Session
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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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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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EFT Session
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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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Precision Session
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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
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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... -
Oscar Jose Pinto Eboli (Federal University of of Rio de Janeiro (BR))
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EFT Session
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Precision Session
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LHCb CollaborationYukawa Session
Thanks to the excellent vertex reconstruction system, the LHCb detector has demonstrated its capabilities in the identification of b- and c-jets.
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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-... -
Precision Session
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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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Precision Session
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Francesco Riva (Universite de Geneve (CH))
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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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Stephen Philip Jones (CERN)
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