Download presentation
Presentation is loading. Please wait.
1
Electroweak and Top Physics at the Tevatron
DIS2000, Liverpool Frédéric Machefert LPNHE-Paris on behalf of the CDF and DØ collaborations Electroweak measurements : W/Z production at the Tevatron W/Z cross-section W width and mass measurements Top quark : Cross-section results Mass measurements Top properties What is expected from Run II ?
2
W / Z production at the Tevatron
Main contribution from QCD cross-section (quark annihilation) p 2 leptons or 2 quarks p Selection on the leptonic decays only Z boson : Require 2 leptons (ee or mm) : Et > GeV Loose id-cuts for 2nd lepton W boson : One isolated lepton (e,m or t) : Et > GeV Neutrino : Et > 25 GeV Electron channel (Run I, L ~ 110 pb-1) : CDF DØ Z candidates W candidates
3
W / Z cross-section Measurement of : swB(Wln) l=e, m, t szB(Z ll)
Dominant uncertainties come from Luminosity Parton Distribution Functions L determined by s(pp) measurements CDF : DL=4.1% (their own meas.) DØ : DL=4.4% (CDF, E710, E811 meas.) L Rel. Diff. of 6.2% 1.062s(DØ) s(CDF) DØ result at s=630 GeV
4
Partial width from Tevatron
BR(W en) Luminosity error vanish From theory : LEP measurement of Partial width from Tevatron
5
Indirect GW measurement
G(Wen) from theory : measured
6
MW measurement Drw : Radiative corrections MW direct measurement :
constraint on MH test of the Standard Model At Tevatron : PZ(n) unknown cannot Measure MW Measure Pt(l) and Mt p p W MT sensitive to Et Pt(l) sensitive to Pt(W) l n Main systematic : lepton energy scale
7
Energy Calibration : CDF
Calibration with Zee and Zmm adjusted to Z mass value Energy scale m momentum linearity low mass resonance :, J/ e energy linearity : E/p E/p ~5 % below expectation (track simulation, radiation, beam constraint)
8
Energy Calibration : DØ
DØ uses electrons only but even at large Calibration with Z ee in CC and EC (limited by Z statistics) MW = 181 MeV (EC) MW = 59 MeV (CC+EC)
9
CDF : MT fit Wen : MW=80.4730.113 GeV Wem : MW=80.4650.143 GeV
Combined result (RunIb /95) : MW(e+m) = 0.089 GeV Combined result (Run 0, Ia, Ib /95): MW(e+m) = 0.079 GeV
10
DØ : MW Combined (CC+EC) MW=80.4800.126 GeV Combined (CC+EC)
Fit of MT : MW=80.7570.230 GeV (EC) Combined (CC+EC) MW=80.7400.097 GeV Fit of pt(e) : MW=80.5470.240 GeV (EC) Combined (CC+EC) MW=80.4800.126 GeV Fit of pt(n) : MW=80.7400.348 GeV (EC) Combined (CC+EC) MW=80.4360.171 GeV Combined result (Run Ia, Ib) : MW = 0.091 GeV
11
MW : World Average (direct measurements)
12
GW direct measurement Transverse Mass Mt depends on G(W)
Fit region Mt > 100GeV : line shape dominates over detector resolution but smaller statistics
13
Results of the fits for GW
CDF (Run Ib) - W en : G(W)=2.170.1250.105 GeV CDF (Run Ib) - W mn : G(W)=1.780.1950.135 GeV CDF Results electron (Ia-Ib) and muon (Ib) : GW = 2.0550.1000.075 GeV
14
Lepton t-e Universality
Ratio of from Luminosity errors cancel t-e universality at 2.5%
15
Top Quark Physics At the Tevatron top quarks are produced by :
quark annihilation (90%) gluon fusion (10%) BR(tbW) ~ 100 % q t b W+ W- l+ n Three types of analysis : dileptons (+2b+2n) lepton + jets all jets Channel BR All jets 44% e+jets 15% m+jets 15% t+X 21% ee 1.2% mm 1.2% em 2.5% b tagging : Soft lepton (CDF+DØ) Displaced vetex (CDF)
16
CDF Top Event tt2b+2jets+e++
17
Top cross-section CDF updated : b-tagging Luminosity
soft lepton tagging No excess
18
Top Mass Procedure : Select top candidates (avoid to bias top mass)
Each event is fitted according to top hypothesis Likelihood fit of Background (QCD, W+jets) + Signal (Herwig) distributions for various values of mtop Fit of Top mass value estimation CDF All jets 6 jets at least 1 SVX Reconstruct mass from best 2
19
CDF : Lepton + jets Isolated lepton (<1) at least 4 jets
Et>20GeV 4 samples : SVX (dble tag) #5 SVX (single tag) #15 SLT (without SVX) #14 no tag #42 4 fits
20
DØ : Dilepton 6 dilepton candidates
Mass weight curves calculated from : Matrix element Neutrino phase space Matrix Element Neutrino Likelihood fit of weight sum :
21
Combined Results Mtop = 174.35.1GeV
22
Constraints on the Higgs mass
MW constraint ~ Mtop constraint
23
Single Top production s channel t channel Signal W+b+b =0.73±0.04pb
Signal W+b+q =1.70±0.09pb Cross-section ~ tt production but huge background 42 events 15 events s < 15.4 pb (95%CL) s < 15.8 pb (95%CL)
24
Top decay in Charged Higgs
Charged higgs Analysis : Appearance / Direct search : look for H+ tn signature (large tanb) Disappearance / Indirect search : deficit of top quark (small & large tanb) Cross-section independent search: deficit of dilepton events w.r.t leptons+jets (small & large tanb - (tt) ind.) (use : Mtop=175 GeV)
25
Z’ & W’ searches - TGC Additional Z ’ and W ’ expected in many extensions of SM Tevatron limits obtained from Dilepton / Dijet events Mass limits depend on the coupling constants 95% C. L. (GeV/c2) L(pb-1) Z’ e+e- > CDF(110) Z’ m + m - > CDF(107) Z’ l+l- > CDF(107) Z, Z, Z , ZI l+l- > 580,610,585,555 CDF(110) ZLR, ZALRM l+l- > 620, 590 CDF(110) W’ en > D0(1a,1b) W’R eNR > D0(1a,1b) W’R eNR > D0(1a,1b) W’ mn > CDF(107) W’ WZ > CDF(90) W’ jj 300 < MW’ <420 CDF(90) WWg / WWZ couplings (LFF = 2 TeV, Dkg=DkZ, lg=lZ) -0.30 < Dk < 0.43 -0.20 < l < 0.20 -0.52 < < 0.78
26
Run II - Upgrade Tevatron - II DØ CDF
Increase energy from 1.8 to 2.0 TeV 2 fb-1 in two years … then 5 fb-1 until LHC ? DØ 2T solenoid 8 layer fiber tracker 4 layer silicon barrel Preshower Extended muon coverage CDF 5 layer double sided silicon barrel Intermediate silicon layers New plug calorimeters extended muon coverage Better m / b-tagging
27
Run II Physics Top Physics : (tt)40% (s ) Mtop ~ 3 GeV
Measurement of tt invariant mass spectrum Measure BR(tWb) to 9% Look for rare decays (limit to BR(tH+b)<11%) Top width to 25% Measurement of |Vtb| ~15 % Each Experiment could reach Mw~ 40 MeV
28
Conclusion Many Results from Run I : Z/W cross-section
Branching Ratios GW and MW measurements Top Discovery Mtop cross-section Top decay In the future (Run II) : W and Top mass combination DMHiggs~ 40%MHiggs Current MW + Mtop - Run II error MHiggs < C.L.
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.