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Di-boson Physics at the TeVatron Andrew Alton University of Michigan CDF Outline Introduction Measurement of W cross section Measurement of Z cross section Measurement of WW cross section

Di-boson Physics at the TeVatron

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Di-boson Physics at the TeVatron. Outline Introduction Measurement of W g cross section Measurement of Z g cross section Measurement of WW cross section WZ(ZZ) cross section limits. Andrew Alton University of Michigan. W. W. Z. W. W. Z. g. Z. g. Diboson Production. - PowerPoint PPT Presentation

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Page 1: Di-boson Physics at the TeVatron

Di-boson Physics at the TeVatronAndrew Alton

University of Michigan

CDF

Outline Introduction Measurement of W cross section Measurement of Z cross section Measurement of WW cross section WZ(ZZ) cross section limits

Page 2: Di-boson Physics at the TeVatron

2Andrew Alton, University of Michigan

Diboson Production

SU(2)LxU(1)Y Electroweak sector non-Abelian theory including boson couplings WW, WWZ (Trilinear gauge boson vertices)

Events with two bosons are sensitive to trilinear gauge boson vertices.

The standard model (SM) has very specific (and small) predictions for the cross section of Di-boson events.

Extensions to the SM often enhance these cross sections. Especially for high boson pt.

Places limits on Anomalous Trilinear Couplings

These final states are backgrounds for other important physics (H->WW, tt->dilepton,etc)

W W

W W

Z Z

Page 3: Di-boson Physics at the TeVatron

3Andrew Alton, University of Michigan

Object Identification

Electrons EM cluster in Cal Et >15 GeV

(often higher 20,25) Track match Shower shape/likelihood CDF - |e| < 1.1, 1.2<|e| <

2.6(2.0) D0 - |e| < 1.1, 1.5<|e| < 2.5

Muons Muon chamber hits Central Track assoc. PT > 20 GeV(15 in Z)

CDF - || < 1.0

D0 - || < 2.0(1.6)

Photons EM cluster in Cal Et >7(8) GeV

CDF(D0) Track veto and isolation Shower shape || < 1.1

Isolated Track Missing Et.

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W Production

W also has an interesting feature interference creates a zero

amplitude in the charge signed rapidity difference between the l and .

Monte Carlo

Page 5: Di-boson Physics at the TeVatron

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W Cross Section

Electron(Muon) Electron(Muon)

Lumi (pb-1) 202(192) 162(82)

ET > 7 GeV > 8 GeV

Tot Bkg 94.7 ± 23.6 124.1 ± 12.5

Candidates 323 223

(pb) 19.7±2.8(stat+sys)±1.1(lum) 19.3±6.7(stat+sys)±1.2(lum)

NLO Theory 19.3 ± 1.4 16.4 ± 0.4

CDF

Page 6: Di-boson Physics at the TeVatron

6Andrew Alton, University of Michigan

Photon Et

Page 7: Di-boson Physics at the TeVatron

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Z Cross Section

Electron(Muon) Electron(Muon)

Lumi (pb-1) 202(192) 177(144)

ET > 7 GeV > 8 GeV

Tot Bkg 4.5 ± 0.8 14.8 ± 1.5

Candidates 70 101

(pb) 5.3±0.7(stat+sys)±0.3(lum) 3.9±0.5(stat+sys)±0.3(lum)

NLO Theory 5.4 ± 0.4 4.3

CDF

Page 8: Di-boson Physics at the TeVatron

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Photon Et

Page 9: Di-boson Physics at the TeVatron

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Two body vs Three Body Mass

Page 10: Di-boson Physics at the TeVatron

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WW Cross Section

Chan ee e All ee e AllBkgd 1.97

0.401.14 0.28

1.66 0.31

4.77 0.70

2.30 0.26

1.94 0.43

3.81 0.30

8.05 0.7

Exp. Sign. *

2.90 0.34

2.75 0.32

5.69 0.66

11.3 1.3

3.26 0.05

2.01 0.05

10.8 0.1

16.1 0.10

Candidates

6 6 5 17 6 4 15 25

CDF

(pp->WW) = 14.3 +5.6 –4.9(Stat) 1.6(sys) 0.9(lum) CDF (lep+trk) = 19.4 5.1(stat) 3.5(sys) 1.2(lum) CDF (dilepton) = 13.8 +4.3 –3.8(Stat) 1.0(sys) 0.9(lum) D0 * CDF uses 13.3 0.8 while

D0 assumes 13.0

Page 11: Di-boson Physics at the TeVatron

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WZ to tri-leptons

D0 looks for W/Z to 3 leptons(e and ). Expects 0.39 0.02 background events Expects 1.02 0.07 signal events (assuming 3.7 pb) Find 1 candidate event. Set upper limit on cross section of 15.1 pb

Page 12: Di-boson Physics at the TeVatron

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Candidate Event

Page 13: Di-boson Physics at the TeVatron

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WZ and ZZ Production

CDF looks for a WZ and ZZ candidates by requiring a Z(ee or ) and Met Significance (sensitive to Z-> and WZ) Or third lepton & MET Or four leptons.

Expect 2.72+-0.33 of signal And 2.29+-0.42 of background Find 4 candidates (all 2 track) Set a limit (ZZ+ZW)<13.9 pb Theory is (ZZ+ZW)=5.2+-0.4 pb

CDF

Page 14: Di-boson Physics at the TeVatron

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Conclusions

Both Tevatron experiments are doing well.

Collection of preliminary cross sections:

Expect limits on anomalous couplings

Analysis using hadron final states underway.

Expect final results and publications soon.