Title: UCLA
1Top Properties at Tevatron Run II 2008
QCD Conference
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Charles Plager UCLA For the CDF and DØ
Collaborations
2New Era of Top Precision Physics!
- CDF and DØ now have more than thirty (30 !!!)
times as much integrated luminosity as we did
when we discovered the top quark in Run I! - With the data we have recorded, we are now able
to have large, very pure top samples. - For example, of the almost 50 results that CDF
sent to the winter conferences, more than half
were in top physics!
Double B-Tag W Jets Candidates
3Top Quark Review
- Fundamental question
- Is it the truth, the Standard Model (SM) truth,
and nothing but the truth? - Did we really find the top quark?
- Is it the SM top quark?
- Is it only the SM top quark?
- The top quark is an ideal place to look for
Beyond the Standard Model Physics!
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tt Pair Lepton Jets Decay
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4What Can We Study About Top Quarks?
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Top physics is very rich.
Branching ratios Rare decays Non-SM decays Decay
kinematics W helicity Vtb
Production cross section Production
mechanism Resonance production Production
kinematics Spin polarization
Top charge Top spin Top mass Top width
In todays talk.
Public Tevatron analyses.
5Top Pair Decay Modes
- According to the SM, top quarks almost (?) always
decay to Wb. - When classifying the decay modes, we use the W
decay modes - Leptonic
- Light leptons (e or ?)
- Tauonic (?)
- Hadrons
6Search for tt Resonances
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- Uses lepton jets
- event selection
- B-tag.
- Invariant mass
- reconstruction
- Assume p?T MET
- Solve for P?z assuming W mass.
- Allows for events with less than three jets.
7Search for tt Resonances, cont.
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- For Z limits, assuming a lepto-phobic Z
- Br (Z ! tt) 100
- MZ gt 760 GeV
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Worlds Most Precise Measurement!
8Search for Invisible Top Decays
- What do we mean by invisible?
- Not (well) reconstructed as double b-tag lepton
jets. - What would happen if there were a large branching
fraction to an invisible decay? For example, - Br (t ! Invisible) 10?
- Br (t ! Wb) 90
- P (tt ! Wb Wb) 81
- ) For a purely invisible decay, we should have
an 19 deficit when we look at the L J event
yield for a given theoretical cross section.
XY
9Feldman-Cousins Acceptance Bands
10Search for Invisible Top Decays, cont.
- From Cacciari et al. (hep-ph 0804.2800)
assuming CTEQ PDFs.
Worlds First Measurement!
11 Search for the Top FCNC Decay t ? Zq
- Top FCNC extremely rare in the SM B(t ? Zq)
O(1014) - Beyond SM B(t ? Zq) up to O(104),
- Any signal at Tevatron or LHC New Physics.
- Signature tt ? Wb Zq (Z 4 Jet).
- Dominant SM background SM Z Jets.
12Search for t ? Zq Ingredients
13Search for t ? Zq Results
- Analysis method Fit mass ?2 in 3 regions
- Signal (B-tagged and Anti b-Tagged)
- Control
- ) Constrain shape normalization of Z jets
background. - Data compatible with background only.
- Feldman-Cousins limit with systematic
uncertainties - 3.5 times better than best
- published limit (L3)
Worlds Best Measurement!
14Looking Forward
- Top quark physics is becoming precision field.
- Almost all analyses (except mass) are still
statistics limited. - So far, most (but not all) things are
frustratingly consistent with the SM. - CDF and DØ each have many of the worlds best
measurments - http//www-cdf.fnal.gov/
- physics/new/top/top.html
- http//www-d0.fnal.gov/Run2Physics/
- WWW/results/top.htm
- MZ (leptophobic) gt 760 GeV (95 C.L.)
- Br (t ! Zq) lt 3.7 (95 C.L.)
- Br (t ! Invisible) lt 9 (95 C.L.)
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- Lots of exciting top physics happening at the CDF
and DØ. - CDF, DØ, and the Tevatron are all running
very well. - A lot of room to grow.
2 fb-1
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15New Era of Precision Top Physics!
2006 PDG Top Entry
2008 PDG Top Entry
2010 PDG Top Entry
16Thank You!
17Backup Slides
18Top Physics Finally Makes Prime Time
The Big Bang Theory! Mondays at 700 on CBS.
Top Branching Fractions
Top FCNC
19(No Transcript)