Title: Tevatron Top Physics
1Tevatron Top Physics
- Meenakshi Narain
- Brown University
- (for the D0 and CDF collaborations)
Fermilab Users Meeting June 4, 2008
2top at Fermilab
- 13 years ago
- we observed a few handfuls of top quark decays
- today
- we are performing detailed studies of 1000s of
top decays
4.2 fb-1
3.7 fb-1
3outline
- strong production
- cross section
- branching fractions
- new physics?
- FCNC decays
- tt resonances
- tb resonances
- H
- .
- electroweak production
- Vtb
4why is the top quark important?
- most massive elementary particle
- dominant contributor to radiative corrections
- how is its mass generated?
- topcolor?
- does it couple to new physics?
- massive G, heavy Z, H,
? mtop2
? log(mH)
5top-antitop production
- strong interaction ? top-antitop pairs
- ? 7.60.6 pb (Kidonakis Vogt,
arXiv0805.3844) - mt 171 GeV, NNLO(approx)NNNLL, CTEQ6M
- ? 7.6 0.6 pb (Cacciari et al.,
arXiv0804.2800) - mt 171 GeV, NLONLL, CTEQ6.5
- ? 7.8 0.6 pb (Moch Uwer, arXiv0804.1476)
- mt 171 GeV, NNLO(approx.), CTEQ6.5
6standard model top decay
- t?Wb with B 100
- W?qq with B 67
- W?l? with B 11
- ??e??/??? with B 17
- final state signatures for top-antitop pairs
primary vertex
secondary vertex
all jets 46
??hadjets 10
dileptons 6
leptonjets 34
??hade/µ 4
7why measure the ttbar cross section?
- cross section analysis
- basic understanding of signal and background
necessary for further study - consistency between channels
- decay branching fractions
- are there non-standard decays?
B(t?Hb) 0
B(t?Hb) 0.1
B(t?Hb) 0.2
B(t?Hb) 0.3
B(t?Hb) 0.4
B(t?Hb) 0.5
B(t?Hb) 0.6
all jets
dileptons
leptonjets
8ttbar cross section in dilepton channel
- characteristics
- small branching fraction
- two neutrinos
- kinematically underconstrained
- signalbackground 31
- selection
- two isolated leptons/leptontrack
- ?2 jets
- missing pT
- Z rejection in ee/?? channels
9ttbar cross section in dilepton channel
- CDF (2 fb-1)
- b-tag
- ? 9.01.1(stat)0.7(syst)0.5(lum) pb
- no b-tag
- ? 6.81.0(stat)0.4(syst)0.4(lum) pb
- D0 (1 fb-1)
- dileptons
- ? 6.81.2-1.1(stat)0.9-0.8(syst)?0.4(lum) pb
- leptontrack
- ? 5.11.6-1.4(stat)0.9-0.8(syst)?0.3(lum) pb
- combined
- ? 6.2 ? 0.9(stat) 0.8-0.7(syst)?0.4(lum) pb
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11ttbar cross section in ? channels
- interesting because of
- t?Hb, H???
- 3 types of hadronic ? decays
- require
- 1 ?, 1 e/?, 2 jets, missing pT
- 1 jet is b-tagged
- neural networks distinguish ? decays from
background
? 7.41.41.3(stat)1.21.1(syst)0.4(lum
) pb (2.2 fb-1) ?B(tt?l?) 0.19?0.08(stat)?0.07(s
yst)?0.01(lum) pb (1 fb-1)
12ttbar cross section in all-jets channel
- characteristics
- large branching fraction
- no neutrinos
- complete reconstruction
- signalbackground 116
- selection
- 6-8 well separated jets
- no significant miss pT
- at least one b-tag
- neural network
- ?ET, event shape, angles
- backgrounds
- pretag data x tagging probability from 4-jet
control region
1 fb-1
CDF PRD 76 072009
? 8.31.0(stat)2.0-1.5(syst)0.5(lum) pb
13ttbar cross section in ljets channel
- characteristics
- large branching fraction
- one neutrino
- kinematically overconstrained
- signalbackground 12, 21(b-tag)
- selection
- one isolated lepton
- 4 jets
- missing pT
14ttbar cross section in ljets channel
- extract top fraction using event topology
- angles, momentum sums, and event shape variables
- dominated by statistical uncertainties
D0 (0.9 fb-1) likelihood discriminant ?6.6?0.8(s
tat)?0.4(syst)?0.4(lum) pb
CDF (0.8 fb-1) neural network ?6.0?0.6(stat)?0.9(
syst)?0.3(lum) pb
15ttbar cross section in ljets channel
- count number of events with at least one b-tagged
jet - smaller statistical uncertainty
- large systematic uncertainty from jet energy
calibration and b-tagging
D0 (0.9 fb-1) ?8.10.5(stat)0.7(syst)
0.5(lum) pb
CDF (2 fb-1) ?8.20.5(stat)0.8(syst)0.
5(lum) pb ?8.71.1(stat)0.9-0.8(syst)0.6(lum)
pb ?7.82.4(stat)1.5(syst)0.5(lumi) pb
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17implications of cross section
- compare different channels
- B(t?Wb)gt0.79 _at_ 95 CL
- B(t?Hb)lt0.35 _at_ 95 CL
- for mH mW and H?cs
- compare with theory
- combine likelihood and b-tag cross section
measurements - stt 7.62 0.85 pb
- for mtop 172.6 GeV
- mt 170 7 GeV
18single top production
- electroweak production of top quarks
- s channel (tb) - t channel (tqb)
- event selection
- 1 isolated e/?
- missing pT
- 2-4 jets, 1 b-tag
NLO ? 0.90.1 pb ? 2.00.3 pb
PRD70 (2004) 114012
19single top production
- D0 results (0.9 fb-1)
- CDF results (2.2 fb-1)
- 4.7 1.3 pb
- significance 2.3 s (expected)
- significance 3.6 s (observed)
- PRL 98, 181802 (2007) PRD (accepted)
- 2.2 0.7 pb
- significance 5.1 s (expected)
- significance 3.7 s (observed)
20single top production
- measure Vtb from total cross section
- D0 Vtbgt0.68 _at_ 95 CL CDF Vtbgt0.66 _at_ 95 CL
- disentangle s and t channels
21top mass measurement
- template fits
- mass estimator (eg best mt from kinematic fitter)
- fit probability density functions from simulated
tt events generated to data
- event-by-event likelihood
- for each event determine likelihood as a function
of mt (eg by integrating over LO matrix
element) - extract mass from peak of joint likelihood
22dilepton channel
- D0 (1 fb-1)
- compute weight curve as a function of top mass
for each event - template fit to mass distribution
- CDF (2 fb-1)
- selection uses evolutionary neural network that
optimizes resolution - compute event weight using LO matrix element
matrix weighting
173.75.4(stat)3.4(syst) GeV
171.22.7(stat)2.9(syst) GeV
23leptonjets
- matrix element analysis
- integrate over LO matrix element to get
likelihood for event as a function of top quark
mass - in situ jet energy calibration using W?qq decay
- peak of joint likelihood top quark mass
- CDF 171.41.5(stat?jes)1.0(syst) GeV (1.9
fb-1) - D0 172.21.1(stat)1.6(syst?jes) GeV (2.1 fb-1)
24all jets (CDF)
- kinematic fitter
- leading 6 jets
- jj/jjj masses, jet pTs
- 2-dimensional template fit
- top/W masses with smallest ?2
mtop 177.0 3.7(stat?jes) 1.6(syst) GeV
25combination
for the first time ?m/mlt1 Run II
goal ?m ? 1 GeV
http//tevewwg.fnal.gov/top/ http//lepewwg.web.ce
rn.ch/LEPEWWG/plots/winter2008/
26top quark couplings
- if top plays a special role in ewk symmetry
breaking its couplings to W bosons may differ
from predictions - sm predicts V-A coupling at Wtb ? helicity of W
boson - F0 0.7, F? 0.3, F 0.0
- (longitudinal, left-handed, right-handed)
- different distributions of ?
- angle between lepton and top in W rest frame
27top quark couplings
- D0 (1 fb-1)
- F0 0.42 ?0.17(stat) ?0.10(sys)
- F 0.12 ? 0.09(stat) ?0.05(sys)
68 CL 95 CL
Phys Rev Lett 100, 062004 (2008)
28searches for non-standard physics
- quarks with charge 4/3e
- FB ttbar asymmetry
- 4th generation t quarks
- scalar top production
- charged Higgs bosons
- tb resonances
- ttbar resonances
- FCNC decays of top quarks
- ? disfavored
- ? consistent with sm
- ? m gt 284 GeV
- no evidence
- limits on H ?tb,t?Hb
29tb resonances
- vector resonance W?tb
- left-handed couplings
- DØ include interference with SM W
- right-handed couplings
- decay to ?Rl/qq, depending on m(?R)
- lower limits on MW 731-825 GeV
30tt resonances
- D0 (2.1 fb-1)
- technicolor Z?tt
- Hill Parke, PRD 49 (1994) 4454)
- CDF (1.9 fb-1)
- massive gluon G?tt
MZgt760 GeV for ?Z/MZ 1.2
31FCNC decays of top quarks
- flavor changing neutral currents
- highly suppressed in sm
- select Z(?ee/??) 4 jets
- fit to
B(t?Zq) lt 3.7 _at_ 95 CL
32conclusion
- top physics has come a long way since 1995
- Tevatron is still the only place to do it
- ttbar cross section measured to 11
- evidence for single top production
- 5? this summer?
- top quark mass measured to 0.8
- will reach uncertainties below 1 GeV
- top properties and possible non-standard physics
studies in great detail - in the last year D0 7 papers and 13 theses
- in the last year CDF 8 papers and 16 theses
- it still looks like top
http//www-d0.fnal.gov/Run2Physics/top/ http//www
-cdf.fnal.gov/physics/new/top/top.html
33thank you
34charged Higgs bosons
- MHgt mt ? H ? tb
- tb resonance
35top quark charge
- is it
- t?Wb (Qtop 2/3 e)
- t?W-b (Qtop -4/3 e)
- Exotic model
- doublet (1/3e,4/3e) ?
- D. Chang et al., PRD59 (1999) 091503
- D0 PRL 98, 041801 (2007)
- 4/3e excluded at 92 CL
- fraction of exotic quark pairs lt 0.80Â Â (90 CL)
- CDF result with 1.5/fb
- p-value for SM 0.31
- exotic model XM excluded with 87 CL
36FB charge asymmetry
- Asymmetry
- LO no asymmetry
- NLO small (3-5) asymmetry predicted in sm
- new physics could lead to larger values (eg Z)
CDF unfold reconstructed AFB to go to parton
level AFBpp 0.17 0.07(stat) 0.04(syst)
D0 AFB in parton rest frame AFB
0.120.08(stat)0.01(syst) consistent with sm
expectation
Phys. Rev. Lett. 100, 142002 (2008)
37t quark
- 4th generation heavy quark
- pair-produced via strong interaction
- more massive than top
- decays to Wb, Ws, Wd
Mt lt 284GeV at 95C.L.
38mass syst
39xsec syst
D0 ljets b-tag kinematic
likelihood