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Don Lincoln, Fermilab
Tales From the FrontA Physicist Reports from the Trenches
Don LincolnFermilab
Don Lincoln, Fermilab
What’s the Point?High Energy Particle Physics is a study of the smallest pieces of matter.
It investigates (among other things) the nature of the universe immediately after the Big Bang.
It also explores physics at temperatures not common for the past 15 billion years (or so).
It’s a lot of fun.
Don Lincoln, Fermilab
Periodic Table
All atoms are madeof protons, neutronsand electrons
Helium Neon
u
du u
d d
Proton NeutronElectron
Gluons hold quarks togetherPhotons hold atoms together
Don Lincoln, Fermilab
Don Lincoln, Fermilab
Now (15 billion years)
Stars form (1 billion years)
Atoms form (300,000 years)
Nuclei form (180 seconds)
Protons and neutrons form (10-10 seconds)
Quarks differentiate (10-34 seconds?)
??? (Before that)
Fermilab4×10-12 seconds
LHC10-13 Seconds
Don Lincoln, Fermilab
Don Lincoln, FermilabIncreasing ‘Violence’ of Collision
ExpectedNumber
ofEvents
Run II
Run I
Increased reach for discovery physicsat highest masses
Huge statistics for precision physicsat low mass scales
Formerly rare processesbecome high statisticsprocesses
1
10
100
1000
The Main Injector upgrade was completed in 1999.
The new accelerator increases the number of possible collisions per second by 10-20.
The major detectors have undertaken massive upgrades to utilize the increased collision rate.
Run II began March 2001
Don Lincoln, Fermilab
Don Lincoln, Fermilab
How Do You Detect Collisions?
• Use one of two large multi-purpose particle detectors at Fermilab (DØ and CDF).
• They’re designed to record collisions of protons colliding with antiprotons at nearly the speed of light.
• They’re basically cameras.
• They let us look back in time.
Don Lincoln, Fermilab
DØ Detector: Run II
30’
30’
50’
• Weighs 5000 tons• Can inspect 3,000,000
collisions/second• Will record 50
collisions/second• Records
approximately 10,000,000 bytes/second
• Will record 1015 (1,000,000,000,000,000) bytes in the next run (1 PetaByte).
Don Lincoln, Fermilab
Highlights from 1992-1996 Run
• Limits set on the maximum size of quarks (it’s gotta be smaller than 1/1000 the size of a proton)
• Supported evidence that Standard Model works rather well (didn’t see anything too weird)
• Studied quark scattering, b quarks, W bosons
• Top quark discovery 1995
Don Lincoln, Fermilab
The Needle in the Haystack: Run I• There are 2,000,000,000,000,000 possible
collisions per second.
• There are 300,000 actual collisions per second, each of them scanned.
• We write 4 per second to tape.
• For each top quark making collision, there are 10,000,000,000 other types of collisions.
• Even though we are very picky about the collisions we record, we have 65,000,000 on tape.
• Only 500 are top quark events.
• We’ve identified 50 top quark events and expect 50 more which look like top, but aren’t.
Run II
×10
Don Lincoln, Fermilab
Top Facts• Discovery
announced March 1995
• Produced in pairs
• Decays very rapidly ~10-24 seconds
• You can’t see top quarks!!!
• Six objects after collision
Don Lincoln, Fermilab
• In each event, a top and anti-top quark is created.
• ~100% of the time, a top quark decays into a bottom quark and a W boson.
• A W boson can decay into two quarks or into a charged lepton and a neutrino.
• So, an event in which top quarks are produced should have:– 6 quarks
– 4 quarks, a charged lepton and a neutrino
– 2 quarks, 2 charged leptons and 2 neutrinos
Top Facts
Don Lincoln, Fermilab
6 quarks
2 quarks2 leptons
2 neutrinos
Taustuff
(hard)
4 quarks1 lepton
1 neutrino
The types ofcollisions one gets
in top-creating collisions are not
unique to top.
In fact, there are many otherways that one can make top-like
collisions.
You have to figure out how to pick the ones you want.
1,000,000 to 1
20 to 1
3 to 1
Top Facts
Don Lincoln, Fermilab
Top Facts• Very messy
collisions
• Hundreds of objects after collision
• Need to simplify the measurement
Don Lincoln, FermilabWe’re in luck!
Quarks can’t exist, except when they are confined
MiracleqAs quarks leave a collision, they change into a ‘shotgun blast’ of particles called a
‘jet’
q
Don Lincoln, Fermilab
Where Did the Energy Go?
Don Lincoln, Fermilab
Combining Viewpoints
Don Lincoln, Fermilab
Measuring Mass: Quicky Review of Special Relativity
For a particle (A), energy, momentum and mass are related:
Let this particle (A) decay into two particles (1) & (2)
High School Physics Energy and momentum are conserved.
222
22242222 1
pEM
MpEc
cMcpE
Lorentz Invariant
221
221
2A
2121
)()(M :So
;
ppEE
pppEEE AA
{ {{Not Lorentz Invariant
Lorentz Invariant
A
1
2
Don Lincoln, Fermilab
The ChallengeEnd on view top + antitop
Algorithm
Algorithm+
Reality
Jets in “God Mode”
Jets in “Don Mode”
Don’t know who goes with what
Know
(1) W + MW2 = (E + E)2 - (p +p)2
(2) Mt = Manti-t
(3) t W + b anti-t W + b jet
jet jet jet
Note:
combinations
121
3
1
4
4 quarks, 1 lepton, 1 neutrino
Guess!!!!
Don Lincoln, Fermilab
Top Quark Run I: The Summary• The top quark was discovered in 1995• Mass known to 3% (the most accurately known
quark mass) • The mass of one top quark is 175 times as heavy
as a proton (which contains three quarks)
Why??
?
Don Lincoln, Fermilab
In 1964, Peter Higgs postulated a physics mechanism which gives all particles their mass.
This mechanism is a field which permeates the universe.
If this postulate is correct, then one of the signatures is a particle (called the Higgs Particle). Fermilab’s Leon Lederman co-authored a book on the subject called The God Particle.
top
bottom
Undiscovered!
Don Lincoln, Fermilab
“LEP observes significant Higgscandidates for a mass of 115 GeVwith a statistical significance of 2.7 and compatible with theexpected rate and distribution ofsearch channels.”
Chris Tully, Fermilab Colloquium13-Dec-2000
Non-Expert Translation:
Maybe we see something, maybe we don’t. The likelihood of error is ~1%.
What we see is consistent with being a Higgs Particle. But it could end up being nothing.
It’s Fermilab’s turn.
Don Lincoln, Fermilab
Higgs Hunting at the Tevatron• If you know the Higgs mass, then
the production cross section and decays are all calculable within the Standard Model– inclusive Higgs cross section is
quite high: • ~ 1pb = 1000 events/year
– but the dominant decay H bb is swamped by background
– thus the best bet appears to be associated production of H plus a W or Z
– leptonic decays of W/Z help give – the needed background rejection
• ~ 0.2 pb = 200 events/year
Don Lincoln, Fermilab
Is a Fermilab Higgs Search Credible?
• LEP incorrect Rule out with 95% certainty by ~2003
• LEP correct Similar quality evidence ~2004-2005 “Discovery” quality evidence ~2007
• Higgs exists but is heavier than LEP suggests Depends on how heavy DØ has a good shot on seeing
‘maybe’ and possibly ‘absolutely’ quality evidence
mH probability density, J. Ellis (hep-ph/0011086)
Don Lincoln, Fermilab
Is a Fermilab Higgs Search Credible?: Good News/Bad News
• Good News ×10 more data than Run I
• Bad News ×1/10 less likely to be created than top quark
• So it’s a wash...similar problem to Run I top search
• Except... Events which look like Higgs but aren’t are much
more numerous. An irony...top quarks are a big piece of the ‘noise’
obscuring Higgs searches.
Don Lincoln, Fermilab
Data-Model Comparison
Don Lincoln, Fermilab
Data-Model Comparison
Don Lincoln, Fermilab
Run II: What are we going to find?
I don’t know!
Improve top quark mass and measure decay modes.
Do Run I more accurately
Supersymmetry, Higgs, Technicolor, particles smaller than quarks, something unexpected?