Masterclass 2011 MINERVA Masterclass ‘Discover the Cosmos’ Teachers’ Workshop 29 th February 2012 Hardeep Bansil.

Slides:



Advertisements
Similar presentations
Masterclass Introduction to hands-on Exercise Aim of the exercise Find out what happens in proton-proton collisions at the LHC as seen by the ATLAS.
Advertisements

Masterclass Introduction to hands-on Exercise Aim of the exercise Identify electrons, muons, neutrinos in the ATLAS detector Types of Events (particles.
Hardeep Bansil Thomas McLaughlan University of Birmingham MINERVA Z Mass Exercise.
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
H1 EventsJoachim Meyer DESY HERA e-p scattering events observed in the H1Detector.
Laura Gilbert How We Study Particles. The basics of particle physics! Matter is all made up of particles… Fundamental particle: LEPTON Fundamental particles:
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Particle Detection and Identification
Detecting Particles Martin Gallacher – University of Birmingham.
ATLANTIS The Event Display for the ATLAS Experiment Qiang Lu, Juergen Thomas, Peter Watkins Particle Physics Group, School of Physics and Astronomy.
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.
ATLANTIS The Event Display for the ATLAS Experiment Qiang Lu, Juergen Thomas, Peter Watkins Particle Physics Group, School of Physics and Astronomy.
More “hands-on” Particle Physics; Learning with ATLAS at CERN Lynne Long, School of Physics & Astronomy, University of Birmingham, Edgbaston, B15 2TT
“Experimental Observation of Isolated Large Transverse Energy Electrons with Associated Missing Energy at = 540 GeV” Okamura Yusuke Shibata lab. G. Arnison.
LHC Detectors 101 Vivek Sharma (with slides stolen from talks of several people ) 1 Good review article: ARNPS 2006, “General purpose detectors for large.
Particle Physics Quiz EPPOG Hands on Particle Physics Masterclasses 2011.
MINERVA Identifying Particle Tracks nneLynne Long University of Birmingham With thanks to Tom McLaughlan & Hardeep Bansil An exercise for students in the.
30 Oct 2009Peter Watkins : Birmingham University1 MINERVA Mark Stockton, Peter Watkins -Birmingham Monika Wielers – RAL Atlantis team - Birmingham, Nijmegen,
Identifying strange particles & determining their properties in the ATLAS experiment People.
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.
Judson Locke, Florida Institute of Technology, Melbourne, Florida, USA Advisor: Richard Teuscher, Ph.D., University of Toronto, Toronto, Ontario, Canada.
Minerva, Feb 9, 2011Monika Wielers (RAL)1 Minerva Abreviation for Masterclass INvolving Event Recognition Visualised with Atlantis developed and 1 st used.
Detecting & observing particles
P ARTICLE D ETECTORS Mojtaba Mohammadi IPM-CMPP- February
Top Quark Lab 15 min YOU 15 min ME 30 min YOU 15 min ME Hand In.
Masterclass Introduction to hands-on Exercise Aim of the exercise  Identify electrons (e), muons (  ), neutrinos( ) in the ATLAS detector  Types.
7 July 2009Neil Collins : University of Birmingham1 MINERVA (Workshop)
W path data analysis International Masterclasses CERN, March 2012.
Masterclass Introduction to hands-on Exercise Aim of the exercise  Identify electrons, muons, neutrinos in the ATLAS detector  Types of Events.
Masterclass 2011 W-Path Data Analysis with MINERVA International Masterclass, CERN 13 th March 2012 Hardeep Bansil.
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.
Identifying strange particles & determining their properties in the ATLAS experiment People.
ATLAS and the Trigger System The ATLAS (A Toroidal LHC ApparatuS) Experiment is one of the four major experiments operating at the Large Hadron Collider.
M. Garcia-Sciveres July 2002 ATLAS A Proton Collider Detector M. Garcia-Sciveres Lawrence Berkeley National Laboratory.
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #9.
ATLAS Z-Path Masterclass Masterclass Analysis Intro.
M.C. Vetterli; SFU/TRIUMF Simon Fraser ATLASATLAS SFU & Canada’s Role in ATLAS M.C. Vetterli Simon Fraser University and TRIUMF SFU Open House, May 31.
H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas
ATLAS and the Trigger System The ATLAS (A Toroidal LHC ApparatuS) Experiment [1] is one of the four major experiments operating at the Large Hadron Collider.
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.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
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.
DE/dx in ATLAS TILECAL Els Koffeman Atlas/Nikhef Sources: PDG DRDC (1995) report RD34 collaboration CERN-PPE
G. Sullivan – Quarknet, July 2003 Calorimeters in Particle Physics What do they do? –Measure the ENERGY of particles Electromagnetic Energy –Electrons,
Measuring the B-meson’s brief but eventful life Tim Adye Rutherford Appleton Laboratory Particle Physics Masterclass th March 2007.
CMS Public Data for High-School Analyses Data Available CMS “Masterclass” Tutorial Resources Dave Barney, CERN 1.
Lecture 18 - Detectors Detector systems
MINERVA.
MINERVA Z Mass Exercise
Introduction to hands-on Exercise
CMS Masterclasses 2017 S’Cool LAB
Charged Current Cross Sections with polarised lepton beam at ZEUS
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
User Guide Tutorial of ISpy and CIMA
How a Particle Detector works
H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas
Measuring the B-meson’s brief but eventful life
CMS Masterclass 2013.
by M. Della Negra, P. Jenni, and T. S. Virdee
The Top Quark Discovery
Project Presentations August 5th, 2004
Charged Current Cross Sections with polarised lepton beam at ZEUS
SUSY SEARCHES WITH ATLAS
Measuring the B-meson’s brief but eventful life
PHYS 3446 – Lecture #18 Monday ,April 9, 2012 Dr. Brandt Calorimeter
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Presentation transcript:

Masterclass 2011 MINERVA Masterclass ‘Discover the Cosmos’ Teachers’ Workshop 29 th February 2012 Hardeep Bansil

Masterclass 2011 Introduction to MINERVA  A masterclass tool for students to learn about the ATLAS Experiment at CERN  Motivates identification of individual particles and events from the signatures seen in the ATLAS detector  Based on the ATLAS event display - Atlantis  Project is a joint venture between the Rutherford Appleton Laboratory (RAL) and the University of Birmingham Masterclass INvolving Event Recognition Visualised with Atlantis

Masterclass 2011 Aims of the exercise  Identify the particles detected by ATLAS detector with the Atlantis Event Display (electrons, muons, neutrinos)  Classify different types of Events (“particles produced in one collision”)  W  e  W   Z  ee  Z   Background from jet production (which might look like W or Z event)  All the above events are ‘well-known’ processes, studied in great detail

Masterclass 2011 How to detect particles in a detector Tracking detector −Measure charge and momentum of charged particles in magnetic field (produced by solenoid) Electromagnetic calorimeter −Measure energy of electrons, positrons and photons Hadronic calorimeter −Measure energy of hadrons (particles containing quarks), such as protons, neutrons, pions, etc. Muon detector −Measure charge and momentum of muons Neutrinos are only detected indirectly via ‘missing energy’ not recorded in the calorimeters Electron Photon Proton or π + Neutrino (not seen) Neutron Muon

Masterclass 2011 GUI Load and cycle through events Control what gets displayed in Canvas Get more details in event

Masterclass 2011 Canvas View event as seen in ATLAS detector in a number of ways Use all views to get the complete picture!

Masterclass 2011 Side view of the detector (R-z projection) Particles in all regions of detector are shown

Masterclass 2011 End-on view of the detector (x-y projection) Warning: Only particles reconstructed in central region shown here (otherwise the particles in the forward would cover the view)!

Masterclass Lego plot (‘rolled out’ calorimeters) Shows energy seen by all regions of the calorimeters as towers

Masterclass 2011 Electron identification Electron deposits its energy in electromagnetic calorimeter Note, what you see here are the energy deposits. Length gives magnitude, but everything is within this calorimeter! Track in tracking detector in front of shower in calorimeter No ‘trace’ in other detectors (electron stops in electromagnetic calorimeter)

Masterclass 2011 Example: W  e Electron track in tracking detector has high “side- ways” or transverse momentum (p T >10GeV) To see this yourself, Electron identification Electron track in tracking detector has high transverse momentum (p T >10GeV) To see this yourself, click on ‘hand’

Masterclass 2011 Example: W  e Electron track in tracking detector has high “side- ways” or transverse momentum (p T >10GeV) To see this yourself, Example: W  e Electron track in tracking detector has high “side- ways” or transverse momentum (p T >10GeV) To see this yourself, click on ‘pick’ Electron identification Electron track in tracking detector has high transverse momentum (p T >10GeV) To see this yourself, click on ‘hand’ move the pointer to the track and click on it

Masterclass 2011 Example: W  e Electron track in tracking detector has high “side- ways” or transverse momentum (p T >10GeV) To see this yourself, click on ‘hand’ move the pointer to the track and click on it Selected track becomes grey Electron identification Electron track in tracking detector has high transverse momentum (p T >10GeV) To see this yourself, click on ‘hand’ move the pointer to the track and click on it Selected track becomes grey p T is shown here

Masterclass 2011 Neutrino identification Characteristics: Neutrino measured indirectly via large missing transverse energy (E T miss > 10GeV) -Red dashed line in end- on view -Note the thickness corresponds to the magnitude of E T miss ( -Not shown if value very small) E T miss value also shown on Lego Plot

Masterclass 2011 Muon identification Track in muon detector Track in tracking detector Extremely small activity in calorimeters Muon has high track transverse momentum (p T >10GeV)

Masterclass 2011 Jet Background Characteristics: Does not contain W  e, W , Z  ee, Z  Typically bundles of particles (jets) are produced Energy deposited in the electro-magnetic and hadronic calorimeter Several tracks belonging to a jet are found in tracking director Missing Energy is usually small or zero

Masterclass 2011 Exercise: Let’s start!  The first event you have to analyse is already displayed  Study each event and classify it into 5 different categories  W  e, W , Z  ee, Z , background  Only one category per event!  There are some additional sheets to help you next to your computer  If you don’t manage to classify all events do not worry!  Have a play with Atlantis  Enjoy and feel free to ask questions!

Masterclass 2011 Exercise: Almost done!  Now capable of identifying different types of events  W  e, W , Z  ee, Z , background  Only worked with a small sample of events  Many more W’s are produced compared to Z events  Note: in reality there many more background events than W or Z events compared to this sample  Thank you for taking part!  Make use of the links available in the handouts (next slide)  Feedback welcome!

19 MINERVA Masterclass Resources Main Minerva website Access to handouts/instruction sheets (also linked from Minerva page under ‘Masterclass resources’) ATLAS Experiment public website Learning with The Particle Adventure (Good introduction to particle physics)