Laura Bernard
(LPSC Grenoble)
27/11/2017 10:30
philippe cotte
(CEA Saclay)
27/11/2017 11:30
Bogna KUBIK
(IPNL)
27/11/2017 14:00
Pierrick Flaux
(LPC Caen)
27/11/2017 14:30
Ahmed Tarek
(LPNHE)
27/11/2017 15:00
Antoine Laudrain
(LAL / U. Paris-Saclay)
27/11/2017 16:00
Peter Falke
(LAPP)
27/11/2017 16:30
Corentin Allaire
(LAL)
28/11/2017 09:30
Dmytro HOHOV
(LAL Université Paris-Sud)
28/11/2017 10:00
Emery Nibigira
(LPC Clermont)
28/11/2017 11:00
chiara amendola
(Laboratoire Leprince-Ringuet, Ecole Polytechnique (FR))
28/11/2017 11:30
Dimitris Varouchas
(LAL-Orsay)
28/11/2017 14:00
Saskia Falke
(LAPP)
28/11/2017 14:30
ilaria luise
(LPNHE)
28/11/2017 15:00
Anyssa Navrer-Agasson
(LPNHE)
28/11/2017 16:30
François Hazenberg
(LPNHE)
29/11/2017 10:00
victoria de Sainte Agathe
(LPNHE)
29/11/2017 11:00
Sylvain Vanneste
29/11/2017 11:30
Nicolas Tonon
(Université de Physique et Ingénierie de Strasbourg)
29/11/2017 16:30
Nihal BRAHIMI
(CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))
29/11/2017 17:00
Hoang Dai Nghia NGUYEN
(CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))
29/11/2017 17:30
Ziyu Guo
(CPPM)
29/11/2017 18:00
Beyhan BASTIN
(GANIL)
30/11/2017 09:30
Valérian Girard-Alcindor
(GANIL)
30/11/2017 11:00
Loïc Le Meur
30/11/2017 11:30
Loic VALERY
(IFAE Barcelona)
01/12/2017 09:00
Thibault Chevalérias
(CEA Saclay)
01/12/2017 09:30
The top quark is the heaviest elementary particle we know. Therefore, it plays a very special role in the Standard Model of particle physics (SM). Its Yukawa coupling to the Higgs boson is close to one, which makes this particle a key element of many Beyond the Standard Model (BSM) theories. The LHC, located at CERN (Geneva, Switzerland) is a proton - proton collider with a center-of-mass...
Albert Druesnes-Saporta
(Institut de Physique Nucléaire de Lyon)
01/12/2017 10:00
I will present the analysis of the μ − e conversion process in a scenario Beyond the Standard Model (BSM), using an effective field theory (EFT) approach. In a first part, I will discuss what is an effective field theory and why we need it. In a second part I will discuss how to use effective field theories to constrain BSM models like μ-e conversion.
Laure MASSACRIER
(Institut de Physique Nucléaire d'Orsay)
01/12/2017 15:30
Frédéric Georges
(IPNO)
01/12/2017 16:00
Amel Belounnas
01/12/2017 16:30
Tasnuva CHOWDHURY
(LPC)
01/12/2017 17:00
Julien MICHAUD
01/12/2017 17:30
Killian Martineau
chiara amendola
(Laboratoire Leprince-Ringuet, Ecole Polytechnique (FR))