Marcel Vreeswijk (Nikhef/UvA-IoP) First Results of ATLAS at the LHC -- The rediscovery of the Standard Model-- Contents: Intro: The Standard Model Elementairy.

Slides:



Advertisements
Similar presentations
B-tagging, leptons and missing energy in ATLAS after first data Ivo van Vulpen (Nikhef) on behalf of the ATLAS collaboration.
Advertisements

1 Beate Heinemann, UC Berkeley and LBNL Università di Pisa, February 2010 Particle Physics from Tevatron to LHC: what we know and what we hope to discover.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Top Physics at the Tevatron Mike Arov (Louisiana Tech University) for D0 and CDF Collaborations 1.
Daniele Benedetti CMS and University of Perugia Chicago 07/02/2004 High Level Trigger for the ttH channel in fully hadronic decay at LHC with the CMS detector.
Experimental aspects of top quark physics Lecture #1 Regina Demina University of Rochester Topical Seminar on Frontier of Particle Physics Beijing, China.
1 Hadronic In-Situ Calibration of the ATLAS Detector N. Davidson The University of Melbourne.
WW  e ν 14 April 2007 APS April Meeting WW/WZ production in electron-neutrino plus dijet final state at CDFAPS April Meeting April 2007 Jacksonville,
Detecting Particles Martin Gallacher – University of Birmingham.
J. Nielsen1 The ATLAS experiment at the Large Hadron Collider Jason Nielsen UC Santa Cruz VERTEX 2004 July 28, 2010.
05/11/2006Prof. dr hab. Elżbieta Richter-Wąs Physics Program of the experiments at L arge H adron C ollider Lecture 5.
Jake Anderson, on behalf of CMS Fermilab Semi-leptonic VW production at CMS.
M. Gilchriese - March 2000 ATLAS at the Large Hadron Collider A Particle Physics Detector at the Energy Frontier M. Gilchriese Lawrence Berkeley National.
prediction-of-higgs-boson.
Wednesday, Apr. 20, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #20 Wednesday, Apr. 20, 2005 Dr. Jae Yu The Standard Model Gauge Bosons Gauge.
August 22, 2002UCI Quarknet The Higgs Particle Sarah D. Johnson University of La Verne August 22, 2002.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
What are we made of ? Neutrinos Building a Particle Collider The ring is 27km round and on average 100m underground CERN – LEP, LHC.
The Discovery of the Top Quark By Ben Smith. Introduction  By 1977, the discovery of the bottom quark suggested the presence of its isospin partner,
1 A Preliminary Model Independent Study of the Reaction pp  qqWW  qq ℓ qq at CMS  Gianluca CERMINARA (SUMMER STUDENT)  MUON group.
Early Electroweak Measurements in CMS and ATLAS J. Alcaraz (CIEMAT - Madrid) XLII Rencontres de Moriond (EW), La Thuile 11 March 2007.
Higgs Properties Measurement based on HZZ*4l with ATLAS
What is the Higgs??? Prof Nick Evans University of Southampton.
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.
1 Top Quark Pair Production at Tevatron and LHC Andrea Bangert, Herbstschule fuer Hochenergiephysik, Maria Laach, September 2007.
C. K. MackayEPS 2003 Electroweak Physics and the Top Quark Mass at the LHC Kate Mackay University of Bristol On behalf of the Atlas & CMS Collaborations.
Sensitivity Prospects for Light Charged Higgs at 7 TeV J.L. Lane, P.S. Miyagawa, U.K. Yang (Manchester) M. Klemetti, C.T. Potter (McGill) P. Mal (Arizona)
QCD at LHC with ATLAS Theodota Lagouri Aristotle University of Thessaloniki (on behalf of the ATLAS collaboration) EPS July 2003, Aachen, Germany.
Discovering the Higgs Boson J. Pilcher Talk for Graduate Students January 9, 2004.
P ARTICLE D ETECTORS Mojtaba Mohammadi IPM-CMPP- February
1 ttbar Cross-Section Studies D. Jana*, M. Saleem*, F. Rizatdinova**, P. Gutierrez*, P. Skubic* *University of Oklahoma, **Oklahoma State University.
H 1 → a 1 a 1 → µ + µ - τ + τ - ATLAS Experiment: Search of Higgs Boson decaying into a 1 in Next to Minimal SuperSymmetric Model By: Hou Keong(Tim) Lou.
Introduction to CERN Activities
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.
Feasibility of Detecting Leptoquarks With the CDF Detector Althea Moorhead Mentor: Darin Acosta.
Emily Nurse W production and properties at CDF0. Emily Nurse W production and properties at CDF1 The electron and muon channels are used to measure W.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Alternatives: Beyond SUSY Searches in CMS Dimitri Bourilkov University of Florida For the CMS Collaboration SUSY06, June 2006, Irvine, CA, USA.
06/30/05 Mathieu Agelou – LowX’05 1 Sensitivity to PDFs at the Tevatron. Mathieu Agelou CEA – Saclay Low x workshop, Sinaia, Romania.
1 Recent results from TEVATRON Yuji Takeuchi (Tsukuba) for CDF and DZero collaborations 16 th YKIS Conference Progress in Particles Physics 2008 Feb. 18.
The Standard Model of the elementary particles and their interactions
M. Garcia-Sciveres July 2002 ATLAS A Proton Collider Detector M. Garcia-Sciveres Lawrence Berkeley National Laboratory.
RECENT RESULTS FROM THE TEVATRON AND LHC Suyong Choi Korea University.
From the Standard Model to Discoveries - Physics with the CMS Experiment at the Dawn of the LHC Era Dimitri Bourilkov University of Florida CMS Collaboration.
Susan Burke DØ/University of Arizona DPF 2006 Measurement of the top pair production cross section at DØ using dilepton and lepton + track events Susan.
1 Measurement of the Mass of the Top Quark in Dilepton Channels at DØ Jeff Temple University of Arizona for the DØ collaboration DPF 2006.
Searching for the Higgs boson in the VH and VBF channels at ATLAS and CMS Dr. Adrian Buzatu Research Associate.
1 Experimental Particle Physics PHYS6011 Fergus Wilson, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2) 3.Collider Experiments.
Régis Lefèvre (LPC Clermont-Ferrand - France)ATLAS Physics Workshop - Lund - September 2001 In situ jet energy calibration General considerations The different.
Z & W Boson Reconstruction with Monte Carlo Simulations and ATLAS DATA Adam Lowery Supervisor: Dr. Jonas Strandberg Wednesday, August 11, 2010.
H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas
CMS Masterclass It’s a time of exciting new discoveries in particle physics! At CERN, the LHC succesfully completed Run I at 8 TeV of collision.
Higgs in the Large Hadron Collider Joe Mitchell Advisor: Dr. Chung Kao.
Searches for Resonances in dilepton final states Searches for Resonances in dilepton final states PANIC th -14 th November 2008, Eilat, ISRAEL A.
FNAL Users’ Meeting– June Fermilab Users’ Meeting CMS Physics from Early LHC Running Dan Green Fermilab For the CMS Collaboration.
LHC Prospects on Standard Model Higgs Riccardo Ranieri INFN and Università degli Studi di Firenze on behalf of ATLAS and CMS Collaborations ICHEP’04 32.
Search for Pair Produced Stops Decaying to a Dileptonic Final State at CMS David Kolchmeyer.
Introduction to Particle Physics II Sinéad Farrington 19 th February 2015.
Suyong Choi (SKKU) SUSY Standard Model Higgs Searches at DØ Suyong Choi SKKU, Korea for DØ Collaboration.
Royal Holloway Department of Physics Top quark pair cross section measurements in ATLAS Michele Faucci Giannelli On behalf of the ATLAS collaboration.
Eric COGNERAS LPC Clermont-Ferrand Prospects for Top pair resonance searches in ATLAS Workshop on Top Physics october 2007, Grenoble.
by M. Della Negra, P. Jenni, and T. S. Virdee
Jessica Leonard Oct. 23, 2006 Physics 835
Observation and measurement of HW+W-
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
Top Quark a particle odyssey Todd Huffman University of Oxford
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
SUSY SEARCHES WITH ATLAS
Susan Burke, University of Arizona
The Top Quark Search Joey Foley.
Presentation transcript:

Marcel Vreeswijk (Nikhef/UvA-IoP) First Results of ATLAS at the LHC -- The rediscovery of the Standard Model-- Contents: Intro: The Standard Model Elementairy particles. Status LHC and ATLAS Physics results 2010

The Standard Model So, what have we been doing in 2010? Measuring ‘backgrounds’! Higgs mechanisme to generate mass! Higgs boson mass > 114 GeV Ultimate goal: detect the Higgs particle (not yet;need more data!)

Marcel Vreeswijk (Nikhef/UvA-IoP) CERN site LHC P+P at 7TeV 27km 60 ton He at 2K 4 big experiments this talk: ATLAS First year of running. (7TeV) high quality data 2010: ~35pb-1 In 2011: run at 7TeV or higher? >>10-fold luminosity? The LUMINOSITY represents the delivered number of proton collisions In addition: Pb+Pb collisions (not in this talk) atlas Large Hadron Collider (LHC)

Marcel Vreeswijk (Nikhef/UvA-IoP) LHC physics reach Production Cross-section of top quarks and W, Z bosons are measurable with 2010 data! Top, W,Z signals are important: 1.Standard candles for calibration 2.Background to new physics & Higgs searches M 5 T # events in 2010 Higgs Top quarks W,Z bosons Proton-Proton In reach in 2010 Higgs W, Z Promising final states: H  W + W -  2 leptons + EtMiss H  ZZ  4 leptons Also H  2 photons 7TeV in 2010 jargon: lepton=electron or muon N = L.  N = # collisions L = Luminosity  = cross-section

Marcel Vreeswijk (Nikhef/UvA-IoP) Inner detector (charged particle tracks) Calorimeter (energy all particles, but muons) Muon ‘Chambers’ ATLAS p Data rec. 93.5% #working channels >99%

Marcel Vreeswijk (Nikhef/UvA-IoP) Performance Inner Tracker 1 m Inner Tracker KsKs    Kaon discovery: 1947 Pixel detector (80M channels) Silicon strips (6M channels) TRT (350k channels) Operational for 97.5% Momentum measurement in magnetic field of 2T Resolution σ(pT)/pT = 0.05%pT ⊕ 1%

Marcel Vreeswijk (Nikhef/UvA-IoP) Performance Calorimeter electromagnetic: Liquid Argon sampling calorimeter. Resolution ~10%/sqrt(E) Granularity: eta x phi=0.025 x    since 1950 Rediscovery of the  0 8m

Marcel Vreeswijk (Nikhef/UvA-IoP) Di-jet physics

Marcel Vreeswijk (Nikhef/UvA-IoP) Di-jet invariant mass New energy domain. Highest Pt jet: 1.12 TeV Highest mass: 3.7 TeV Searches for new physics ongoing ATLAS published 3 papers on jet measurements pp jet

Marcel Vreeswijk (Nikhef/UvA-IoP) Performance Muons Physics signals show up! Muon system: 1200 Muon chamber 350k drift tubes (air core toroidal field 0.5T) Designed for TeV muons (not yet) Z boson ‘rediscovered’ Originally: 1983 at CERN Mass: GeV

Marcel Vreeswijk (Nikhef/UvA-IoP) Muon resonances ATLAS 2010   ? mass Published 2010 Z cross-section in new energy domain=7TeV

Marcel Vreeswijk (Nikhef/UvA-IoP)  Missing Transverse energy W boson ‘rediscovered’ Originally: 1983 at CERN Mass: 80.4 GeV

Marcel Vreeswijk (Nikhef/UvA-IoP) W boson production W decays to muon + (unseen) neutrino.  Missing transverse energy.  W q q’ g Transverse W mass:

Marcel Vreeswijk (Nikhef/UvA-IoP) Top pair (ttbar) production complicated events: 1.Many jets with 2 b-jets (can be ‘tagged’) 2.Electron or Muon 3.EtMiss  Standard candle  New physics may show up p p t t ttbar has two measurable decays modes:  single-lepton  di-lepton (mode is set by W decay) ttbar single-lepton Datum Basic prper. Europ. Topds! Last heaviest known particle Last before new

Marcel Vreeswijk (Nikhef/UvA-IoP) di-leptonic ttbar 2 b-tagged jets

Marcel Vreeswijk (Nikhef/UvA-IoP) ttbar More info on poster by Ido & Hegoi N. from Nikhef Van Tera naar 100evts selectie Speld hooi

Marcel Vreeswijk (Nikhef/UvA-IoP) ttbar: theory & experiment

Marcel Vreeswijk (Nikhef/UvA-IoP) Higgs in 2011 ? We have measured the ‘backgrounds’, now we are ready for the signal ! Conclusion The LHC and the ATLAS detector have demonstrated to be ready for the Standard Model Higgs or new physics See next talk by Paul de Jong!

Marcel Vreeswijk (Nikhef/UvA-IoP) BACKUP “We know everything about the Higgs boson except its mass” Λ (GeV) Higgs mass (GeV) Triviality Vacuum stability Limits on m h from theory Limits on m h from exper.

Marcel Vreeswijk (Nikhef/UvA-IoP) W boson cross section

Marcel Vreeswijk (Nikhef/UvA-IoP) Photon production (QCD compton) photons of hundreds of GeVs ! (Xray GeV)

Marcel Vreeswijk (Nikhef/UvA-IoP)

The Standard Model Ultimate goal: detect the Higgs particle (not yet…need more data!) So, what have we been doing in 2010? Measuring ‘backgrounds’! + Higgs boson to generate mass! Promising decay modes H  2 photons H  W+W-  2 leptons + EtMiss H  ZZ  4 leptons and much more….

Marcel Vreeswijk (Nikhef/UvA-IoP) The Standard Model Production Cross-section of top quarks and W, Z bosons are measurable with 2010 data! Top, W,Z signals are important: 1.Standard candles for calibration 2.Background to new physics & Higgs searches M 5 T # events in 2010 Higgs Top quarks W,Z bosons Proton-Proton In reach in 2010 Note: a proton=many quarks+gluons Higgs W, Z Promising final states: H  W + W -  2 leptons + EtMiss H  ZZ  4 leptons Also H  2 photons 7TeV in 2010 jargon: lepton=electron or muon

Marcel Vreeswijk (Nikhef/UvA-IoP) CERN site LHC P+P at 7TeV 27km 60 ton He at 2K 4 big experiments this talk: ATLAS First year of running. (7TeV) high quality data 2010: ~35pb-1 This year (2011): run at 7TeV or higher? >>10-fold luminosity? The LUMINOSITY represents the delivered number of proton collisions 3.2T botsingen 655k hi Pb=Pb

Marcel Vreeswijk (Nikhef/UvA-IoP) Z boson production  Do we understand Z production and its backgrounds?  First measurement ever at 7 TeV. Ook in e+e- Diagrammen Lin schaal? Datum Z massa 2Gev wordt 90GeV