-
Thomas Mueller (CNRS / IN2P3 / LLR)27/11/2017 10:00
-
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
-
Julien Masbou (SUBATECH)28/11/2017 16:00
-
Anyssa Navrer-Agasson (LPNHE)28/11/2017 16:30
-
Joao Da Rocha28/11/2017 17:00
-
Julien Masbou (SUBATECH)29/11/2017 09:30
-
François Hazenberg (LPNHE)29/11/2017 10:00
-
victoria de Sainte Agathe (LPNHE)29/11/2017 11:00
-
Sylvain Vanneste29/11/2017 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
-
Simon Giraud30/11/2017 10:00
-
Valérian Girard-Alcindor (GANIL)30/11/2017 11:00
-
Loïc Le Meur30/11/2017 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...
Go to contribution page -
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.
Go to contribution page -
Clement Leloup01/12/2017 11:00
In order to solve the hierarchy problem and to answer the question “what is Dark Matter ?”, many models involving additional spatial dimensions have been proposed. Among them is the branon model, which predicts the production of branons, scalar Dark Matter candidates, along with Standard Model particles. This study proposes to search for branon production at center of mass 13 TeV in hadronic...
Go to contribution page -
Gaël Touquet (IPNL)01/12/2017 11:30
Le Modèle Standard décrit les constituants élémentaires de la matière ainsi que les forces fondamentales leur permettant d'interagir : électromagnétisme, interaction nucléaire forte, et interaction nucléaire faible. Le boson de Higgs est la pierre angulaire du modèle standard pour deux raisons. D'une part, le champ de Higgs provient de la brisure spontanée de la symétrie électrofaible et il...
Go to contribution page -
Joao Coelho (LAL)01/12/2017 13:30
-
Vitalii LISOVSKYI (LAL)01/12/2017 14:00
In the Standard Model (SM) of particle physics, the couplings of gauge bosons to the charged leptons of different generations are predicted to be identical, up to the order of mass-related corrections. This property is known as Lepton Universality (LU), and an observation of LU violation should be a sign of the New Physics (NP). A variety of tests of LU was performed in the past, generally...
Go to contribution page -
Daniel Cuesta (IPHC-DRS)01/12/2017 14:30
Dans le contexte actuel de recherche de physique au-delà du modèle standard de la physique des particules, l’expérience Belle II s’apprête à enregistrer ses premières collisions au printemps 2018 à KEK au Japon. Son objectif est d’observer des manifestations quantiques extrêmement rares de processus de nouvelle physique dans le secteur des saveurs de quarks et de leptons chargés. Cela...
Go to contribution page -
Laure MASSACRIER (Institut de Physique Nucléaire d'Orsay)01/12/2017 15:30
-
Frédéric Georges (IPNO)01/12/2017 16:00
-
Amel Belounnas01/12/2017 16:30
-
Tasnuva CHOWDHURY (LPC)01/12/2017 17:00
-
Julien MICHAUD01/12/2017 17:30
-
William Barbe (LPC Clermont)
-
Killian Martineau
-
chiara amendola (Laboratoire Leprince-Ringuet, Ecole Polytechnique (FR))
Choisissez le fuseau horaire
Le fuseau horaire de votre profil: