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Thomas Mueller (CNRS / IN2P3 / LLR)11/27/17, 10:00 AM
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Laura Bernard (LPSC Grenoble)11/27/17, 10:30 AM
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philippe cotte (CEA Saclay)11/27/17, 11:30 AM
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Bogna KUBIK (IPNL)11/27/17, 2:00 PM
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Pierrick Flaux (LPC Caen)11/27/17, 2:30 PM
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Ahmed Tarek (LPNHE)11/27/17, 3:00 PM
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Antoine Laudrain (LAL / U. Paris-Saclay)11/27/17, 4:00 PM
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Peter Falke (LAPP)11/27/17, 4:30 PM
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Corentin Allaire (LAL)11/28/17, 9:30 AM
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Dmytro HOHOV (LAL Université Paris-Sud)11/28/17, 10:00 AM
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Emery Nibigira (LPC Clermont)11/28/17, 11:00 AM
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chiara amendola (Laboratoire Leprince-Ringuet, Ecole Polytechnique (FR))11/28/17, 11:30 AM
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Dimitris Varouchas (LAL-Orsay)11/28/17, 2:00 PM
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Saskia Falke (LAPP)11/28/17, 2:30 PM
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ilaria luise (LPNHE)11/28/17, 3:00 PM
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Julien Masbou (SUBATECH)11/28/17, 4:00 PM
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Anyssa Navrer-Agasson (LPNHE)11/28/17, 4:30 PM
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Joao Da Rocha11/28/17, 5:00 PM
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Julien Masbou (SUBATECH)11/29/17, 9:30 AM
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François Hazenberg (LPNHE)11/29/17, 10:00 AM
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victoria de Sainte Agathe (LPNHE)11/29/17, 11:00 AM
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Sylvain Vanneste11/29/17, 11:30 AM
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Nicolas Tonon (Université de Physique et Ingénierie de Strasbourg)11/29/17, 4:30 PM
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Nihal BRAHIMI (CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))11/29/17, 5:00 PM
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Hoang Dai Nghia NGUYEN (CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))11/29/17, 5:30 PM
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Ziyu Guo (CPPM)11/29/17, 6:00 PM
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Beyhan BASTIN (GANIL)11/30/17, 9:30 AM
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Simon Giraud11/30/17, 10:00 AM
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Valérian Girard-Alcindor (GANIL)11/30/17, 11:00 AM
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Loïc Le Meur11/30/17, 11:30 AM
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Loic VALERY (IFAE Barcelona)12/1/17, 9:00 AM
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Thibault Chevalérias (CEA Saclay)12/1/17, 9:30 AM
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...
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Albert Druesnes-Saporta (Institut de Physique Nucléaire de Lyon)12/1/17, 10:00 AM
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.
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Clement Leloup12/1/17, 11:00 AM
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...
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Gaël Touquet (IPNL)12/1/17, 11:30 AM
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...
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Joao Coelho (LAL)12/1/17, 1:30 PM
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Vitalii LISOVSKYI (LAL)12/1/17, 2:00 PM
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...
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Daniel Cuesta (IPHC-DRS)12/1/17, 2:30 PM
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...
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Laure MASSACRIER (Institut de Physique Nucléaire d'Orsay)12/1/17, 3:30 PM
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Frédéric Georges (IPNO)12/1/17, 4:00 PM
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Amel Belounnas12/1/17, 4:30 PM
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Tasnuva CHOWDHURY (LPC)12/1/17, 5:00 PM
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Julien MICHAUD12/1/17, 5:30 PM
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William Barbe (LPC Clermont)
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Killian Martineau
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chiara amendola (Laboratoire Leprince-Ringuet, Ecole Polytechnique (FR))
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