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top quark mass measurements at the Tevatron. Ulrich Heintz Boston University (for the D0 and CDF collaborations). XLIII Rencontres de Moriond, QCD and High Energy Interactions, La Thuile, March 8-15, 2008. t. W. W. b. H 0. W. W. introduction. - PowerPoint PPT Presentation
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top quark mass measurements at the Tevatron
Ulrich Heintz
Boston University(for the D0 and CDF collaborations)
XLIII Rencontres de Moriond, QCD and High Energy Interactions, La Thuile, March 8-15, 2008
3/11/2008 Ulrich Heintz - Moriond QCD 2
introduction• top is the most massive fundamental particle
• dominant contributor to radiative corrections
W W
t
b
W W
H0
mtop2
log(mH)
3/11/2008 Ulrich Heintz - Moriond QCD 3
top production and decay• production
– pp tt with ≈ 7 pb
• decay – tWb with B ≈ 100% – Wqq with B ≈ 67 %– Wℓ with B ≈ 11%
e with B ≈ 17 %
• final state signatures for top-antitop pairs
• b-tagging
lepton+jets38%
dilepton 6%
all jets56%
primaryvertex
secondary vertex
3/11/2008 Ulrich Heintz - Moriond QCD 4
jet energy scale/combinatorics/radiation• calibrate jet response
– external calibration– in situ calibration
• W qq from top decays
• many jets– combinatorics
• how to associate them with partons from top decay?
– initial state and final state radiation
• which jets are from top decay?
3/11/2008 Ulrich Heintz - Moriond QCD 5
template fits• mass estimator
– typically best mtop from kinematic fitter
• templates– probability density functions from simulated tt events
generated with a range of top quark mass values
• maximum likelihood fit– fit templates to data distribution
• ensemble test validation– perform analysis many times on pseudodata sets
generated to have same signal/background as expected in collider data
– average and rms of measured mass– correct for biases
3/11/2008 Ulrich Heintz - Moriond QCD 6
matrix element method• probability density for event o if top quark mass is mt
• signal probability
• combine all events in a joint likelihood
• and maximize wrt mt jes ftop
jesbkgtopjestsigtoptopjestevt opfmopffmoL |1,|,,|
topjesti
n
i
topjestn fmoLfmooL ,,|ln,,|ln1
1
top fraction jet scale parameter
jestttttt
jestsig qoWmqdxfxfxdxdm
mop
,|,1
,|
normalization pdf |M|2 dLIPS
detector response function
3/11/2008 Ulrich Heintz - Moriond QCD 7
dileptons• characteristics
– small branching fraction– two neutrinos– kinematically
underconstrained + signal:background = 3:1+ combinatorics: 2
• selection– two isolated leptons 2 jets
– miss pT
– Z rejection in ee/ channels
Dilepton(BR~6%)
e,
b-jet
e,
b-jet
miss pT
Dilepton(BR~6%)
e,
b-jet
e,
b-jet
e,
b-jet
e,
b-jet
miss pT
3/11/2008 Ulrich Heintz - Moriond QCD 8
dileptons (D0 – 1.05 fb-1)• matrix weighting
– for each top mass determine possible top/antitop momenta
– weight by pdf, probability for lepton energy
• template fit– top mass with largest weight
• neutrino weighting– for each top mass loop over
neutrino pseudorapidities – weight by consistency with
observed missing pT,
• template fit– mean and rms of weight curves
57/13 eventsmatrix weighting
3/11/2008 Ulrich Heintz - Moriond QCD 9
dileptons (D0 – 1.05 fb-1)• statistical correlation factor = 0.67
matrix weighting: 175.2±6.1(stat)±3.4(syst) GeVweighting: 172.5±5.8(stat)±3.5(syst) GeVcombined: 173.7±5.4(stat)±3.4(syst) GeV
3/11/2008 Ulrich Heintz - Moriond QCD 10
dileptons (CDF)• matrix element (2.0 fb-1)• selection uses evolutionary
neural network that optimizes resolution
weighting (1.9 fb-1)• template fit to mass with
largest weight and to HT
171.2±2.7(stat)±2.9(syst) GeV 171.6±3.3(stat)±3.8(syst) GeV
344/192 events
144/34 events
3/11/2008 Ulrich Heintz - Moriond QCD 11
lepton+jets• characteristics
+ large branching fraction+ one neutrino+ kinematically overconstrained + signal:background = 1:2, 2:1(b-tag)– combinatorics: 12, 6(1 b-tag), 2(2 b-tags)
• selection– one isolated lepton – 4 jets
– miss pT
– at least one b-tag jet
e,
b-jet
b-jet
jet
Lepton+jets(BR~38%)
miss pT
jet
e,
b-jet
b-jet
jetjet
e,
b-jet
b-jet
jet
Lepton+jets(BR~38%)
miss pT
3/11/2008 Ulrich Heintz - Moriond QCD 12
lepton+jets (D0 – 2.1 fb-1)• matrix element analysis – calibrate with pseudodata sets
• Run IIa: 170.5 ± 2.5(stat jes) ± 1.4 GeV (0.9 fb-1) • Run IIb: 173.0 ± 1.9(stat jes) ± 1.0 GeV (1.2 fb-1) • combined:172.2 ± 1.1(stat) ± 1.6 GeV (2.1 fb-1)
271/109 events
3/11/2008 Ulrich Heintz - Moriond QCD 13
lepton+jets (CDF – 1.9 fb-1)• matrix element signal likelihood• NN discriminant gives event-by-event background fraction• no integration over background matrix elements• subtract expected background contribution from likelihood
172.7±1.8 (statjes)±1.2(syst) GeV
318/70 events
3/11/2008 Ulrich Heintz - Moriond QCD 14
lepton+jets (CDF – 1.9 fb-1)• template fit to mtop and mjj from kinematic fit
mtop= 171.8 ± 1.9 (statjes) ± 1.0 (syst) GeV
332/47 events
3/11/2008 Ulrich Heintz - Moriond QCD 15
all jets (CDF)• characteristics
+ large branching fraction+ no neutrinos+ complete reconstruction– signal:background 1:16– combinatorics 90/30(1 tag)/6(2 tags)
• selection– 6-8 well separated jets– no significant miss pT
– at least one b-tag– neural network
• kinematic fitter– leading 6 jets– jj/jjj masses, jet pTs– use top/W masses with smallest 2
• background model– pretag data * tagging probability
jet
b-jetb-jet
jet
jet jet
All-hadronic(BR≈56%)
3/11/2008 Ulrich Heintz - Moriond QCD 16
all jets (CDF – 1.9 fb-1)• 2-dimensional template fit
mtop = 177.0 ± 3.7(statjes) ± 1.6(syst) GeV 3112/2570 events
3/11/2008 Ulrich Heintz - Moriond QCD 17
combinationRun IIMeasurement
CDF di-l
D0 di-l
CDFl+j
D0l+j
CDFall-j
CDFlxy
worldaverag
e
∫Ldt (fb-1) 2.0 1.1 1.9 2.1 1.9 0.7
Result 171.2 173.7 172.7 172.2 177.0 180.7 172.6
Jet Energy Scale 2.5 3.1 1.5 1.3 2.0 0.3 0.9
Signal 0.7 0.8 0.6 0.7 0.6 1.4 0.5
Background 0.4 0.6 0.6 0.4 1.0 7.2 0.4
Fit 0.6 0.9 0.2 0.1 0.6 4.2 0.1
MC 0.7 0.2 0.4 0.0 0.3 0.7 0.2
Systematic 2.8 3.4 1.7 1.6 2.4 8.5 1.1
Statistical 2.7 5.4 1.2 1.1 3.3 14.5 0.8
Total Uncertainty 3.9 6.4 2.1 1.9 4.1 16.8 1.4
•statistical: uncorrelated•jet energy scale: several subcategories with different correlations•signal: ISR, FSR, pdf, b-id – correlated for all•background: correlated within channels•fit: MC stats – uncorrelated•MC: Monte Carlo generator – correlated for all
3/11/2008 Ulrich Heintz - Moriond QCD 18
combination
GeV 1.38.169
GeV 5.14.172
GeV 9.33.177
TeV-EWWG
http://tevewwg.fnal.gov/top/
3/11/2008 Ulrich Heintz - Moriond QCD 19
winter 2008 global electroweak fit• LEP EWWG procedure
• results for winter 2008 (summer 2007) had = 0.02767±0.00034
s = 0.1185±0.0027
– MZ = 91.1874±0.0021 GeV
– mtop = 172.8±1.4 GeV (171.3±1.7 GeV)
– MH = 87 +36 -27 GeV (76 +33 -24 GeV)
2/dof = 17.2/13 (18.2/13)– p-value = 19%
3/11/2008 Ulrich Heintz - Moriond QCD 20
winter 2008 global electroweak fit
mH < 160 GeV @ 95% C.L. (<190 GeV incl. LEP-2 limit)
LEP-EWWG procedure
http://lepewwg.web.cern.ch/LEPEWWG/plots/winter2008/
3/11/2008 Ulrich Heintz - Moriond QCD 21
conclusions• with 2 fb-1
– mtop = 172.6 ± 1.4 GeV
m/m = 0.8%
• with full data set (8 fb-1)– experimental precision
below 1 GeV– push on systematics
• are we missing anything?– color reconnections– what are we measuring?
• MC top mass parameter• pole mass?
http://www-d0.fnal.gov/Run2Physics/top/http://www-cdf.fnal.gov/physics/new/top/top.html