QuarkNet Beyond the First Year

Slides:



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

The Standard Model and Beyond [Secs 17.1 Dunlap].
ATLAS Experiment at CERN. Why Build ATLAS? Before the LHC there was LEP (large electron positron collider) the experiments at LEP had observed the W and.
1 Analysis of Prompt Diphoton Production at the Large Hadron Collider. Andy Yen Mentor: Harvey Newman Co-Mentors: Marat Gataullin, Vladimir Litvine California.
Quark Net 2010 Wayne State University Physics Department.
Nailing Electroweak Physics (aka Higgs Hunting) with the Next Linear Collider Bob Wilson High Energy Physics Group CSU Physics Research Evening November.
8/5/2002Ulrich Heintz - Quarknet Particle Physics what do we know? Ulrich Heintz Boston University.
Particle Physics From Strings To Stars. Introduction  What is Particle Physics?  Large Hadron Collider (LHC)  Current Experiments – ALICE – ATLAS –
Particle Physics at the Energy Frontier Tevatron → LHC & The Very Early Universe Tony LissAir Force Institute of TechnologyApril 10, 2008.
Nuclear Physics A Glimpse into the Quantum Universe Ramone Brown, Solomon Utain Mentor: Dr. Richard Jones Nuclear Physics 1.
US CMS Colloquium: Dec., The Physics of the LHC The Compact Muon Solenoid at the Large Hadron Collider Dan Green Fermilab US CMS Project Manager.
QuarkNet Presentation B. Beiersdorf, South Bend LaSalle High School and Notre Dame QuarkNet Center 1 QuarkNet: Exploring the Frontiers of High Energy Physics.
Particle Physics J4 Leptons and the standard model.
The Higgs Boson: without the maths and jargon David Hall Graduate Seminar Series St Catherine’s College MCR 11 th May 2011.
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.
My Chapter 30 Lecture.
Point 1 activities and perspectives Marzio Nessi ATLAS plenary 2 nd October 2004 Large Hadron Collider (LHC)
August 22, 2002UCI Quarknet The Higgs Particle Sarah D. Johnson University of La Verne August 22, 2002.
1 FK7003 Elementary Particle Physics David Milstead A4:1021 tel: /
Standard Model A Brief Description by Shahnoor Habib.
1 Experimental HEP at Syracuse Marina Artuso Steven Blusk Tomasz Skwarnicki Sheldon Stone Postdoctoral Researchers Graduate StudentsResearch Professors.
QuarkNet July 2010 Najla Mackie & Tahirah Murphy.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
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.
Introduction to Particle Physics How to compute the Universe?
A Brief Introduction to Quarknet and Particle Physics Mike Strauss.
7 July 2009Neil Collins : University of Birmingham1 MINERVA (Workshop)
Re-creating the Big Bang Experiments at the Large Hadron Collider Dr Cormac O’ Raifeartaigh (WIT) Albert Einstein Ernest Walton.
Introduction to CERN Activities
H. Dauerty Attracting HS Student Participation in HEP AAPT Meeting 11 Ja2001nuary Attracting High School Student Participation in Particle Physics Research.
The ATLAS Experiment; to the Heart of Matter The SFU Experimental High-Energy Particle Physics Group 3 faculty members, 3 postdocs, 7-8 graduate students,
QuarkNet Mentor Presentation – April 24, 2002 B. Beiersdorf, QuarkNet Staff Teacher 1 Beth Beiersdorf Fermilab QuarkNet – Beyond the First Year.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Compelling Scientific Questions The International Linear Collider will answer key questions about matter, energy, space and time We now sample some of.
ELECTROWEAK UNIFICATION Ryan Clark, Cong Nguyen, Robert Kruse and Blake Watson PHYS-3313, Fall 2013 University of Texas Arlington December 2, 2013.
The Standard Model of the elementary particles and their interactions
1 The Standard Model of Particle Physics Owen Long U. C. Riverside March 1, 2014.
Particle Detectors January 18, 2011 Kevin Stenson.
J.4.1State the three-family structure of quarks and leptons in the standard model. J.4.2State the lepton number of the leptons in each family. J.4.3Solve.
H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas
880.P20 Winter 2006 Richard Kass 1 Detector Systems momentumenergy A typical detector beam looks something like: BaBar, CDF, STAR, ATLAS, GLAST…… particle.
G. Sullivan – Quarknet, July 2003 Calorimeters in Particle Physics What do they do? –Measure the ENERGY of particles Electromagnetic Energy –Electrons,
Steve Chao & Maha Hamid. Day 1 After reviewing the syllabus for the two weeks, we moved to laboratory to take apart and rebuild two cosmic ray detector.
Standard Model of Particle Physics
LECTURE 9 Chasing Relativistic Particles
The Discovery of THE HIGGS BOSON Why is it Exciting?
Elementary Particle Physics
The Standard Model of Particle Physics
QuarkNet Beyond the First Year
A Brief Introduction to Quarknet and Particle Physics
Introduction to CERN Activities
From Before… Essay Due Today Discussed the weak interaction
The Standard Model strong nuclear force electromagnetic force
H Y P A T I A HYbrid Pupil’s Analysis Tool for Interactions in Atlas
The Compact Muon Solenoid at the Large Hadron Collider
Elementary particles Spring 2005, Physics /24/2018 Lecture XXV.
B. Beiersdorf, QuarkNet Review, Dec 2001
Particle Physics what do we know?
Particle Physics Part 1 -James Joyce Contents: Particle Accelerators
Particle physics.
History of Particle Nuclear Physics!
Radiation Shield Design by UA
Particle Physics and The Standard Model
Beyond the standard model
SPH4U Elementary Particles.
Subatomic Particles and Quantum Theory
The Standard Model By: Dorca Lee.
Beyond the Higgs wan ahmad tajuddin wan abdullah
SUSY SEARCHES WITH ATLAS
Vision A community of researchers including faculty, postdoctoral, graduate and undergraduate students and high school teachers and high school students.
Presentation transcript:

QuarkNet Beyond the First Year What happens next? What?!! A 3-week workshop! My experience at Notre Dame QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

What happens next? QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

You’ve mentored 2 high school physics teachers. You’ve spent 7 weeks teaching new researchers. You’ve answered a zillion questions about physics, particle physics and “classroom transfer.” You’ve learned a bit about how the “usual” high school physics class is taught. That wasn’t so bad . . . QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Now you get to: Recruit 10 more teachers Plan and implement a 3-week workshop Find speakers Figure out what “classroom transfer” means Reserve rooms, labs Pay 10 more teachers Schedule activities for 3 weeks Keep up with 12 total teachers through the academic year QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

What?!! A 3-week workshop! QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Lead teachers and mentors plan Associate Teacher Institute together. ATI is parallel to the Lead Teacher Institute but sensitive to local teachers’ needs. Approximately 10 associate teachers join the Center. Largest group of teachers added to QuarkNet Center. QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Associate Teacher Institute 10 Associate Teachers 2 Mentors 2 Lead Teachers Associate Teacher Institute QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

The ATI program is research-based; for example, experimenting with cosmic ray detectors. Some groups complete detectors and then use them in their classrooms. QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Each center hosts a two to three week Associate Teacher Institute (100 hours minimum) Generally, institutes meet for three 5-day weeks or two 5-day weeks with plans to meet on five Saturdays (or holidays) during the academic year. QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

My Experience at Notre Dame QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Vision A community of researchers including high school teachers, faculty, postdocs, graduate and undergraduate students and high school students. QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Recruiting Meeting, Fall 1999 QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

Fermilab QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

The e- was discovered by Thompson ~ 1900 The e- was discovered by Thompson ~ 1900. The nucleus was discovered by Rutherford in ~ 1920. The e+, the first antiparticle, was found in ~ 1930. The m , indicating a second “generation”, was discovered in ~ 1936. There was an explosion of baryons and mesons discovered in the 1950s and 1960s. They were classified in a "periodic table" using the SU(3) symmetry group, whose physical realization was point-like, strongly-interacting, fractionally-charged "quarks." Direct evidence for quarks and gluons came in the early 1970s. The exposition of the 3 generations of quarks and leptons is only just, in 1996, completed. In the mid 1980s, the unification of the weak and electromagnetic force was confirmed by the W and Z discoveries. The LHC, starting in 2005, 2006, 2007?, 2008? will be THE tool to explore the origin of the breaking of the electroweak symmetry (Higgs field?) and the origin of mass itself. QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

E2 = p2c2 + m2c4 New Physics: Higgs Bosons Supersymmetry String Theory A key equation: E2 = p2c2 + m2c4 New Physics: Higgs Bosons Supersymmetry String Theory Hidden Dimensions looking for particles based on energy, momentum and mass QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

The D detector has 3 main detector systems; ionization tracking, liquid argon calorimetry ( EM , e , and HAD , jets), magnetized steel + ionization tracker and muon detection/identification. This event has jets, a muon, an electron and missing energy , n. QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

SM Fundamental Particle Appears As   (ECAL shower, no track) e e (ECAL shower, with track)   (ionization only) g Jet in ECAL+ HCAL q = u, d, s Jet (narrow) in ECAL+HCAL q = c, b Jet (narrow) + Decay Vertex t --> W +b W + b e Et missing in ECAL+HCAL -->l +  +l Et missing + charged lepton W --> l + l Et missing + charged lepton, Et~M/2 Z --> l+ + l- charged lepton pair --> l + l Et missing in ECAL+HCAL QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

QuarkNet Mentor Presentation – April 22, 2003 Research next QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

QuarkNet Mentor Presentation – April 22, 2003 choosing students QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member

QuarkNet After the First Year Things change – 2nd, 3rd, 4th, 5th, etc. Research and classroom become foci Communication leads to teachers becoming members of the particle physics community Collaboration formed – mentor(s)-teacher(s) QuarkNet Mentor Presentation – April 22, 2003 B. Beiersdorf, QuarkNet Staff Member