H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas

Slides:



Advertisements
Similar presentations
Hardeep Bansil Thomas McLaughlan University of Birmingham MINERVA Z Mass Exercise.
Advertisements

Basic Measurements: What do we want to measure? Prof. Robin D. Erbacher University of California, Davis References: R. Fernow, Introduction to Experimental.
Detecting Particles Martin Gallacher – University of Birmingham.
 Stable and unstable particles  How to observe them?  How to find their mass?  How to calculate their lifetime? 6/9/
CMS Masterclass. It’s the dawn of an exciting age of new discovery in particle physics! At CERN, the LHC and its experiments are underway. ATLAS and.
CMS Masterclass It’s a time of exciting new discoveries in particle physics! At CERN, the LHC and its experiments are underway. ATLAS and CMS, the.
10/2/2015C.Kourkoumelis,UoA1 WP3 Educational and Outreach Portal C. Kourkoumelis, UoA.
1 A Preliminary Model Independent Study of the Reaction pp  qqWW  qq ℓ qq at CMS  Gianluca CERMINARA (SUMMER STUDENT)  MUON group.
“Experimental Observation of Isolated Large Transverse Energy Electrons with Associated Missing Energy at = 540 GeV” Okamura Yusuke Shibata lab. G. Arnison.
MINERVA Identifying Particle Tracks nneLynne Long University of Birmingham With thanks to Tom McLaughlan & Hardeep Bansil An exercise for students in the.
Z boson mass reconstruction Caroline Steiblin Prof. Al Goshaw Dr. Andrea Bocci Duke University 1.
Study of the to Dilepton Channel with the Total Transverse Energy Kinematic Variable Athens, April 17 th 2003 Victoria Giakoumopoulou University of Athens,
Masterclass Introduction to hands-on Exercise Aim of the exercise  Identify electrons (e), muons (  ), neutrinos( ) in the ATLAS detector  Types.
30/Jul/20101 Research of Z generation Ken-ichiro KOIKE.
Masterclass Introduction to hands-on Exercise Aim of the exercise  Identify electrons, muons, neutrinos in the ATLAS detector  Types of Events.
Feasibility of Detecting Leptoquarks With the CDF Detector Althea Moorhead Mentor: Darin Acosta.
ATLAS Z-Path Masterclass It’s a time of exciting new discoveries in particle physics! At CERN, the LHC and its experiments are underway. The ATLAS.
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.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Masterclass 2011 MINERVA Masterclass ‘Discover the Cosmos’ Teachers’ Workshop 29 th February 2012 Hardeep Bansil.
SEARCH FOR AN INVISIBLE HIGGS IN tth EVENTS T.L.Cheng, G.Kilvington, R.Goncalo Motivation The search for the Higgs boson is a window on physics beyond.
ATLAS Z-Path Masterclass Masterclass Analysis Intro.
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.
Marcel Vreeswijk (Nikhef/UvA-IoP) First Results of ATLAS at the LHC -- The rediscovery of the Standard Model-- Contents: Intro: The Standard Model Elementairy.
W. Riegler/CERN History of Instrumentation ↔ History of Particle Physics The ‘Real’ World of Particles Interaction of Particles with Matter Tracking Detectors,
W. Riegler/CERN History of Instrumentation ↔ History of Particle Physics The ‘Real’ World of Particles Interaction of Particles with Matter Tracking Detectors,
W. Riegler/CERN History of Instrumentation ↔ History of Particle Physics The ‘Real’ World of Particles Interaction of Particles with Matter Tracking Detectors,
Introduction to Particle Physics II Sinéad Farrington 19 th February 2015.
XLIX International Winter Meeting on Nuclear Physics January 2011 Bormio, Italy G. Cattani, on behalf of the ATLAS Collaboration Measurement of.
1 E T miss measurement E T miss is an important signal for - new physics (e.g. SUSY, H  ZZ  ll ) - reconstruction of a narrow invariant mass distribution.
Lecture 18 - Detectors Detector systems
MINERVA.
Analyzing ATLAS Data Name: Manuel / Kit TRUIMF UBC MasterClass
Žilina, Z path with ATLAS data Ivan Melo.
MINERVA Z Mass Exercise
Introduction to hands-on Exercise
QuarkNet Beyond the First Year
CMS Masterclass 2012.
CMS Masterclasses 2017 S’Cool LAB
WP3 Educational and Outreach Portal
CMS Masterclass 2012.
User Guide Tutorial of ISpy and CIMA
G. Arnison et al., UA1 Collaboration
Tatia Engelmore, Columbia University
Inside the Tevatron Main Ring
How a Particle Detector works
Elementary particles Spring 2005, Physics /24/2018 Lecture XXV.
Xinyu Miao Department of Physics Univ. of Arizona 03/30/07
CMS Masterclass 2013.
by M. Della Negra, P. Jenni, and T. S. Virdee
Particle physics.
The Top Quark Discovery
Top Quark Production at the Large Hadron Collider
Particle physics at the LHC and ATLAS.
Missing Energy and Tau-Lepton Reconstruction in ATLAS
Jessica Leonard Oct. 23, 2006 Physics 835
Subatomic Particles and Quantum Theory
CMS Masterclass 2017.
More leptons.
Real Life I BUBBLES! ICECREAM theory.
SUSY SEARCHES WITH ATLAS
ATLAS Z-Path Masterclass 2011
Z path with ATLAS data Ivan Melo
ATLAS Z-Path Masterclass Start-up
Particles going through matter
C.M.S.:.
The Top Quark Search Joey Foley.
The Higgs Boson Science Volume 338(6114): December 21, 2012
Presentation transcript:

H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas http://hypatia.phys.uoa.gr/applet

First woman mathematician Alexandria, Egypt (370-418 A.D.) HYPATIA of Alexandria First woman mathematician Alexandria, Egypt (370-418 A.D.)

Collisions Energy of each beam 3,5 TeV 2 x 3.5 TeV = 7 TeV Some of the particles produced are unstable and decay immediately

ATLAS Particle tracks appear as lines on the detectors The length of each track is determined by particle type Each particle leaves a trace only on specific detectors according to its type

HY.P.A.T.I.A. Track Momenta Histograms Displays the quantities that describe each track (type, momentum, charge, φ, θ) Histograms Created automatically from the tracks of the invariant mass table

HY.P.A.T.I.A. Invariant Mass Η → 4ℓ Main event analysis window. Displays the user selected tracks from various events. Calculates invariant masses. Creates Histograms. Η → 4ℓ

Laboratory Exercise

Detection and mass calculation of Z bosons Real Events Laboratory Exercise Detection and mass calculation of Z bosons Real Events Z → μ- + μ+ Z → e- + e+ 2 tracks, opposite charge, not diametrical Invariant mass 91,2 GeV Small missing energy ETMiss Background events Leptons from quark decays are in jets Cosmic rays : diametrical tracks on both detector views Large missing energy ETMiss (because of neutrinos)

Laboratory Exercise Recognition of electrons - muons e : charged particles, usually isolated that leave a trace in the E/M calorimeter μ : charged particles that leave a trace in the muon chambers

Laboratory Exercise Detection and mass calculation of Z bosons - Histogram

Laboratory Exercise Discover the Higgs H → 2 Z → 4l Z → e- + e+ or Z → μ- + μ+ H  2 e- + 2 e+ H  2 μ- + 2 μ+ Η  e- + e+ + μ- + μ+ Isolated tracks 6 GeV Cut 4-track Invariant mass Not real Higgs, mass 180 GeV

Track Examples

Laboratory Exercise