8.882 LHC Physics
Experimental Methods and Measurements
Introductory Lecture
[Lecture 1, February 4, 2009]
Physics
Colloquium Series The Physics Colloquium Series
‘09
Spring
Thursday, February 5 at 4:15 pm in room 10-250
Paul Canfield Iowa State University
"Ending of the Tyranny of Copper: Intermetallic Superconductivity in the Post Copper-oxide Age"
For a full listing of this semester’s colloquia, please visit our website at
web.mit.edu/physics
Lecture Outline Introduction of Course Personnel Objective of this Course Organization of the Lectures ● Prerequisites ● Schedule:
lectures and recitations ● Course grade
Course Content Overview Overview of LHC Project and Physics C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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The Lecturer T
Christoph Paus
physics career
started PhD 1992 at L3 (e+e--, LEP, CERN) in 1998 moved to CDF (pp, TeVatron, FNAL) since 2006 mostly CMS (pp, LHC, CERN)
physics measurements
precision electroweak (Z boson mass & width, EWK parameters) B physics directly related to CKM matrix (Standard Model) Standard Model Higgs boson search contact interactions, magnetic monopoles, pentaquarks, excited onia
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Objective of this Course - 8.882 O
Course focus introduce experimental methods perform typical measurements at the LHC and TeVatron
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Not the purpose of this course
provide fully fledge theoretical background
quantum field theory courses good for that also nuclear and particle physics standard g raduate courses
provide in depth discussion of how detectors work
nuclear and particle physics standard graduate courses maybe specialized course for detector design and construction
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Goal in practical terms learn how to do research as an experimentalist at LHC be prepared to go to CERN and start an analysis .. or at least know how experimentalists try to do their job
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Organization of the Course O
Prerequisites ● special
relativity, quantum physics ● good to have heard particle physics 1+2 but not needed g
Dates ● Monday,Wednesday ● it
1:00pm – 2:30pm (Kolker room)
seems Monday/Wednesday 2:00pm – 3:30pm fits better
● recitation
to be arranged with recitation instructor, TBA ● office hours to be arranged (appointment per e-mail) ● video office hours very useful and easy to setup v
Execution ● most
lectures will be taught over video
● third
time done at MIT, nevertheless nothing is set in stone ● open to changes of course setup according to your comments C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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Organization of the Course Execution continued ● participation
from outside MIT/CERN welcome (see FNAL) ● lecture slides will be available from the Web ● core of the course are four analyses, performed by you ●3
use real CDF data (Ebeam= 1 TeV) ● 1 uses Monte Carlo simulation of CMS detector (Ebeam= 5-7 TeV) ● recommended
to pair up and work together ● analyses have to be handed in as short notes ● conference at the end of the course, one topic per student
Course grade ● basis:
3 analyses notes and final project presentation
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Technicalities T
Access to computers get account at MIT Tier 2 center request account: http://www.lns.mit.edu/compserv/cms-acctappl.html
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Access to course documentation and “log book” we use a TWiki to run and document the course try it as your personal “log book” example: user = ChristophPaus (yours will be equivalent)
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Video tools for remote participants: use EVO at evo.caltech.edu register and follow instructions to start EVO tools
before we used VRVS, EVO is still new, but worked quite well
details explained on the course TWiki
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Course Content C
Five big blocks introduction and overview charged track multiplicity measurement upsilon cross section measurement B meson lifetime measurement Standard Model Higgs searches
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Lecture plan not exactly cast in stone if you have special wishes let me know
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Course Content: First Block •
Introduction and overview introductory lecture accelerators particle detectors overview
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Course Content: Second Block •
Charge track multiplicity measurement heavy ion physics overview charge multiplicity measurements data analysis strategies and essentials detectors: tracking track reconstruction and fitting analysis tips – charge multiplicity
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Course Content: Third Block •
Upsilon cross section, production fractions onia as probes in heavy ion physics secondary particle production detectors: electrons, muons and particle Id analysis tips – bottomonia cross section resonances production, decay and reconstruction search strategies and observations efficiency and acceptance
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Course Content: Fourth Block •
B meson lifetime measurement high energy physics overview b hadron lifetimes and other essentials B physics trigger studies proper time reconstruction sophisticated selections: likelihood/neural networks
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Course Content: Fifth Block •
Standard Model Higgs searches Higgs search and other essentials detectors: calorimetry jets and missing energy B tagging review
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Interesting Material I
Videos: academic lectures and presentations CERN: http://webcast.cern.ch/home/pages/archive_cds.php SLAC: http://www-conf.slac.stanford.edu/ssi FNAL: http://www-visualmedia.fnal.gov/ check the archives
Wikipedia LHC: http://en.wikipedia.org/wiki/Large_Hadron_Collider CMS: http://en.wikipedia.org/wiki/Compact_Muon_Solenoid CDF: http://en.wikipedia.org/wiki/Collider_Detector_at_Fermilab also try google, YouTube etc. fantastic documentation on the Web though, read with care
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References will be provided throughout the course C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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The Large Hadron Collider (LHC) T
Most important features
proton-proton collider Ebeam= 7 TeV (TeV Vatron: 1 TeV) heavy ion (Pb, Ca) collider E = 5.5 TeV beam instantaneous luminosity: 1034 cm2s-1 (TeVatron: 1032cm2s-1) bunch spacing: 25 ns (TeVatron: 396 ns)
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Main physics goals discover the Higgs or falsify the Standard Model search for direct signals of New Physics
LHC party line schedule (delays still quite possible)
Aug 2009: single beam run at Ebeam = 7 TeV Sep 2009: first collisions at E = 7 TeV, low lumi 15x15 beam last year: Sep 2008 all was ready but an incident stopped running the machine
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Overview: CERN (Geneva, Switzerland) Check out serious YouTube: CERN LHC 2007 http://youtube.com/watch?v=s9XotvwgnaY
France 6 mile s
Gene va ai rport
Switzerland
: Check out fun YouTube: Day to Day Communications (1974) http://youtube.com/watch?v=OymJC9KkWlg
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The LEP/LHC Tunnel Setup Tunnel is 27 km long 50-150m below ground
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The LEP/LHC Tunnel Setup Tunnel is 27 km long 50-150m below ground
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LEP Tunnel before LHC
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Empty Tunnel: LEP Disassembled
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The LHC Dipoles
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LHC Pictures: Simulation
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LHC Pictures: Real Dipoles
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LHC Pictures: Tunnel with Beamlines
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LHC Experiments L
Two omnipurpose* detectors Atlas CMS
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One dedicated B physics experiment
LHCb L
One dedicated heavy ion experiment
Alice A
* omnipurpose = do heavy ion and B physics as well C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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The LHC Experiments
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Alice: The Mission Statement •
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The ALICE Collaboration is building a dedicated heavy-ion detector to exploit the unique physics potential of nucleus-nucleus interactions at LHC energies. Our aim is to study the physics of strongly interacting matter at extreme energy densities, where the formation of a new phase of matter, the quark-gluon plasma*, is expected.
* today we know the fireball (plasma) behaves more like a fluid than a gas C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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Alice: Detector Sketch old L3 magnet
particle physicists do recycle C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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Alice: December 2006
April, 2007
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Atlas/CMS Motivation A
LHC is a new energy regime: uncharted territory u
The guaranteed mission (seek and destroy) find the Standard Model Higgs: completes SM, for now do not find the SM Higgs: falsify the model because machine fully covers available phase space
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The case for beyond the Standard Model new energy regime opens new doors anything beyond the Standard Model is a sensation be it SUSY, extra dimensions, leptoquarks, Z', .... or even better: the completely unexpected
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Atlas: Detector Sketch
the biggest collider detector ever, by far eye catcher: central air core toroid magnet
7,000 ton weight, 25 m diameter, 45 m long
light weight construction: if wrapped in plastic it floats on water (22,000 m3) still, weights more than half the Eiffel tower C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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Atlas: Real Installation
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CMS – Compact Muon Solenoid 12,500 ton weight, 15 m diameter, 22 m long
compact does not mean small volume smaller than Atlas by ~5.6, but weights 30% more than the Eiffel tower eye catcher: brilliant design in separately removable slices C. Paus, Lecture 8.882 – LHC Physics: Introductory Lecture
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CMS: Installation
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LHCb: Mission and Sketch •
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The Large Hadron Collider beauty experiment for precise measurements of CP violation and rare decays
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LHCb: At the Interaction Point
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CDF: Sketch
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CDF Detector Pictures D i12mx12mx16m m e n s i o n s
Dimension:
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CDF: Time Of Flight Detector scintillation bars holders photomultiplier
happy MIT folks cone
pre-amp
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CDF: Central Outer Tracker
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CDF: Central Outer Tracker
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CDF: Silicon Detector
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CDF: Silicon Vertex Detector
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Pointers to Interesting Video Material P
Overview of the engineering design of CMS
http://cmsinfo.cern.ch/outreach/CMSmedia/CMSmovies.html >> http://cmsinfo.cern.ch/outreach/CMSmedia/Movies/CMSTheMovie.mpg >> http://cmsinfo.cern.ch/outreach/cmseye/yb0_lowering.htm
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Conclusions C
Instructions for course get registered for a user account on the computing center try out your TWiki account think about good time for Recitation Sessions check out the Web site
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Course overview it is going to be an exciting course please be interactive the last two years the course was a full success still, we need your help us make it best for this year
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Plan for Next Lecture •
Accelerators basic physics of accelerators design parameters of accelerators hadron versus electron colliders examples of accelerators today what is the future of accelerators?
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Last Year's Recitation Instructor L
Michael Miller
physics career
started at MSU next Yale (heavy ion: RHIC, STAR) now MIT (heavy ion: STAR, neutrino: SNO)
physics measurements
jet quenching (STAR) gluon helicity distribution in pp collisions jet cross sections in pp collisions total solar neutrino flux
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He is faculty in Seattle now....
if you can find him he is very knowledgeable
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