UCLA High Energy & Astro-Particle (HEAP) Seminar

Slides:



Advertisements
Similar presentations
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
Advertisements

Ken Bell – Rutherford Appleton Laboratory
First results from the ATLAS experiment at the LHC
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
Top Physics at the Tevatron Mike Arov (Louisiana Tech University) for D0 and CDF Collaborations 1.
Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u.
Physics with ATLAS and CMS Are there new symmetries or extra-dimensions? What is dark matter? Where does mass come from? The two big multi-purpose experiments.
1 Hadronic In-Situ Calibration of the ATLAS Detector N. Davidson The University of Melbourne.
Fabiola Gianotti, Physics at LHC, Pisa, April 2002 PART 2.
J. Nielsen1 The ATLAS experiment at the Large Hadron Collider Jason Nielsen UC Santa Cruz VERTEX 2004 July 28, 2010.
New Physics at the LHC/ILC B-L Workshop, LBNL September, 2007 Sally Dawson (BNL)
LHC’s Second Run Hyunseok Lee 1. 2 ■ Discovery of the Higgs particle.
Sung-Won Lee 1 Study of Jets Production Association with a Z boson in pp Collision at 7 and 8 TeV with the CMS Detector Kittikul Kovitanggoon Ph. D. Thesis.
prediction-of-higgs-boson.
Reconstruction of High Transverse Momentum Top Quarks at CMS Gavril Giurgiu (Johns Hopkins University) For the CMS Collaboration 2009 DPF Meeting Wayne.
August 22, 2002UCI Quarknet The Higgs Particle Sarah D. Johnson University of La Verne August 22, 2002.
FNAL Academic Lectures – May, –Tevatron -> LHC Physics 3 –Tevatron -> LHC Physics 3.1 QCD - Jets and Di - jets 3.2 Di - Photons 3.3 b Pair Production.
Working Group C: Hadronic Final States David Milstead The University of Liverpool Review of Experiments 27 experiment and 11 theory contributions.
Higgs Properties Measurement based on HZZ*4l with ATLAS
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
Report from India Topical Conference on Hadron Collider Physics XIII Jan 14-20, TIFR, India Naohito Saito RIKEN/ RIKEN BNL Research Center.
FSU Experimental HEP Faculty Todd Adams Susan Blessing Harvey Goldman S Sharon Hagopian Vasken Hagopian Kurtis Johnson Harrison Prosper Horst Wahl.
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
ATLAS Z-Path Masterclass It’s the dawn of an exciting age of new discovery in particle physics! At CERN, the LHC and its experiments are tuning.
Top Quark Physics At TeVatron and LHC. Overview A Lightning Review of the Standard Model Introducing the Top Quark tt* Pair Production Single Top Production.
Jonathan Nistor Purdue University 1.  A symmetry relating elementary particles together in pairs whose respective spins differ by half a unit  superpartners.
Abstract Several models of elementary particle physics beyond the Standard Model, predict the existence of neutral particles that can decay in jets of.
A. Bertolin on behalf of the H1 and ZEUS collaborations Charm (and beauty) production in DIS at HERA (Sezione di Padova) Outline: HERA, H1 and ZEUS heavy.
ATLAS Z-Path Masterclass Masterclass Analysis Intro.
Standard Hadron Colliders III. Triple Bosons & Top Quark P.Mättig Bergische Universität Wuppertal Peter Mättig, CERN Summer Students 2014.
Top Higgs Yukawa Coupling Analysis – Status Report Hajrah Tabassam Quai-i-Azam University, Islamabad ON BEHALF OF: R. Yonamine, T. Tanabe, K. Fujii, KEK.
Tao Han* Muon Collider as a Higgs Factory Pittsburgh Particle physics, Astrophysics & Cosmology Center University of Pittsburgh ICFA Workshop, HF 2012.
Marcel Vreeswijk (Nikhef/UvA-IoP) First Results of ATLAS at the LHC -- The rediscovery of the Standard Model-- Contents: Intro: The Standard Model Elementairy.
Introduction to Particle Physics II Sinéad Farrington 19 th February 2015.
Determining the CP Properties of a Light Higgs Boson
Electroweak physics at CEPC
Searching for New Exotic Physics at the LHC
Boosted Higgs  bb in association with a vector boson, at 14 TeV
Current status and future prospects
Missing Transverse Energy Calibration in W/Z(+jets) Events
The ATLAS Experiment at the LHC
UCLA High Energy & Astro-Particle (HEAP) Seminar
UCLA High Energy & Astro-Particle (HEAP) Seminar
Harvard ATLAS CERN LHC A general purpose detector designed to study proton-proton collisions at the CERN Large Hadron Collider (LHC) in Geneva,
The Era of Discovery at the Large Hadron Collider
Xinyu Miao Department of Physics Univ. of Arizona 03/30/07
Special UCLA High Energy & Astro-Particle (HEAP) Seminar
UCLA High Energy & Astro-Particle (HEAP) Seminar
UCLA High Energy & Astro-Particle (HEAP) Seminar
CMS Physics Analysis in China
Xinyu Miao Department of Physics Univ. of Arizona 03/30/07
Particle Physics Theory
UCLA High Energy & Astro-Particle (HEAP) Seminar
Particle physics at the LHC and ATLAS.
UCLA High Energy & Astro-Particle (HEAP) Seminar
CMS Masterclass 2017.
Physics at the Tevatron: Lecture I
University of Tsukuba, Japan Particle Physics Phenomenology,
Are you ready to speak English?
Are you ready to speak English?
New Physics at a TeV and the LHC – II & III
E. Richter-Was, Institute of Physics UJ
CMS Physics Analysis in China
Are you ready to speak English?
TeV Physics and ILC 何红建 清华大学.
SUSY SEARCHES WITH ATLAS
ATLAS Z-Path Masterclass 2011
Composite Weak Bosons LHC.
ATLAS Z-Path Masterclass Start-up
Search for a New Vector Resonance in the pp WWtt+X Channel at LHC
Presentation transcript:

UCLA High Energy & Astro-Particle (HEAP) Seminar “Discovery and Precision: The two faces of the LHC physics in the coming years” Presented by Michail Bachtis, CERN The discovery of the Higgs boson in the first run of the LHC constitutes a triumph of the Standard Model (SM) of particle physics. The priority of the LHC experiments in Run II is to look for deviations of the SM by directly searching for new physics at the new center of mass energy of 13 TeV. A direct search for TeV resonances decaying into a pair of bosons (W,Z,H) where at least one of them decays into jets will be presented. In this boosted regime, the jets are merged into a broad jet. Jets from bosons need to be separated from QCD jets and the techniques used open a new chapter in theory and experiment known as jet substructure. In case of no discoveries at the LHC, the scale of new physics needs to be probed by precision measurements that are very challenging in a hadron collider. One of the most important measurements to be performed at the LHC is the measurement of the mass of the W boson. The prospects of performing such measurement will be described with emphasis on the experimental challenges and especially on calibrating the momentum scale of 40 GeV muons with a precision of some MeV. Location: PAB 4-330 Date: Thursday, March 3rd, 2016 Time: 12:30pm Refreshments at 12:15pm