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Recent Results on Electroweak

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24 April 2003 - DIS03 - St. Petersburg, Russia. Alan L. Stone - Louisiana Tech University ... data taken from mid-August '02 through mid-January 03. Integrated ... – PowerPoint PPT presentation

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Title: Recent Results on Electroweak


1
Recent Results on Electroweak Related Physics
at DØ
2
Motivation for Measuring W Z Production
  • Test of SM couplings
  • Constrain proton PDFs
  • Probe effects of NLO QCD corrections
  • Better understanding of our Experiment
  • Efficiencies, Backgrounds, Luminosity
  • Use these signals to tune triggers algorithms
  • Improved luminosity measurement
  • With sufficiently small statistical systematic
    uncertainties
  • Normalize to other measurements
  • Preliminaries to other Run II goals
  • W boson mass
  • Precision EW measurements
  • Top Quark Studies
  • (W or Z) Higgs

3
W and Z Production Mechanics
4
W Z Cross Sections A Counting Experiment
5
The DØ Run II Detector
6
The Muon Detector
  • Two regions Three layers of Scintillators and
    Drift Tubes
  • Central and Forward
  • A ? inside toroid magnet
  • B C ? outside toroid magnet
  • Muon rapidity coverage to 2
  • Shielding reduces backgrounds by 50-100x

7
Z 0mm Event Selection
8
Z0mm Efficiencies
mcontrol
(scaled)
Z
mprobe
(scaled)
9
Z0mm Cross Section
  • Drell-Yan Contribution
  • Correct for 121 due to photon exchange and
    photon-Z interference determined from Pythia

10
W0mn Event Selection
11
W0mn Cross Section
12
The Calorimeter
  • Liquid argon sampling
  • Stable, uniform response, rad. hard
  • LAr purity important (lt 0.7 ppm O2 equivalent)
  • Uranium absorber (Cu/Fe for coarse hadronic)
  • dense absorber hence can be compact
  • Nearly compensated EM and hadronic response
  • Linear response
  • Hermetic with full coverage
  • h lt 4.2 (q 2o)
  • l int gt 7.2 (total)

13
W/Z0e Event Selection
14
Z0ee Cross Section
D0 Run II Preliminary
  • Drell-Yan Contribution
  • Small effect (1.7) in the mass window of 70 lt
    mee lt 110 GeV
  • QCD Background
  • Determined from data by fitting signal and
    background shape

Mee-(GeV)
15
W0en Backgrounds
  • Dominant background from QCD multijet events
  • Estimated from data

Solve for NW
From QCD dijet sample
D0 Run II Preliminary
D0 Run II Preliminary
2.3/-1
16
W0en Cross Section
17
Results
Z
W
C. R. Hamberg, W.L. van Neerven and T. Matsuura,
Nucl. Phys. B359 (1991) 343
CTEQ4M PDF
18
Direct Search for Z'ee
  • Search for Non-SM heavy particles that decay to
    lepton pairs
  • Assumes Z' couples as Z
  • Previous Tevatron Run I Limit
  • MZ'gt690 GeV
  • Event Selection
  • 2 isolated EM objects
  • hlt1.1 or 1.5lthlt2.5
  • ETgt25 GeV
  • No track requirement necessary

D0 Run II Preliminary
M(ee) around the Z
Data Bkg (QCDDY/Z) Bkg (QCD only) 10x Z'(600GeV)
Mee-(GeV)
19
Z? Search
  • Form limit from the ratio of cross sections for
    (sB)Z'/(sB)Z where many of the systematic errors
    in the efficiencies and luminosity measurements
    cancel
  • Applied a binned likelihood approach with Poisson
    statistics
  • Remaining Uncertainties
  • K-factor 5
  • Az?/Az PDFs 2-3

20
  • Run I Discovery
  • stt
  • Top mass
  • W helicity in top events
  • tt spin correlations
  • Top pT
  • Searches for new physics
  • (X tt and top decay)
  • Run II With high precision we hope to answer
    questions such as
  • Why is top so heavy?
  • Is it or the third generation special?
  • Is top involved with EWSB?
  • Is it connected to new physics?

21
Top Quark Production Mechanics
  • At the Tevatron, top quarks are produced in pairs
  • Br(t?Wb)100

22
s(ttlljets) Event Selection
  • Event Selection
  • Two high pT isolated m or e
  • ET (Z mass) cut
  • ? 2 jets, ETgt20 GeV h lt 2.5
  • HT S(ElT ,EjetT) cut
  • Backgrounds
  • WW, Z? tt determined with MC
  • Z/g, Wjets and QCD from data

D0 Run II Preliminary
ET (GeV)
mmjets
e
Di-muon mass (GeV)
23
s(ttlljets) Results
D0 Run II Preliminary
emjets
Jet1
Jet2
emjets
D0 Run II Preliminary
Jet Multiplicity
24
s(ttljets) Event Selection (no m tag)
  • Procedure
  • Preselect a sample rich in W?s
  • Evaluate QCD multi-jet (as f Njets )
  • Estimate W4 jets assuming Berends Scaling
  • Apply topological selection
  • Event Selection
  • Isolated lepton w/ PTgt20 GeV
  • MET gt 20 GeV
  • 4 jets with ETgt15 GeV hlt2.0 (2.5)
  • Soft non-isolated muon tag veto
  • Backgrounds
  • multijet evaluated from data vs. Njets
  • ejets due to fake jets (real po and g)
  • mjets due to heavy flavor decays
  • Estimate real W4 jets with scaling law

Estimation of QCD Background
D0 Run II Preliminary
a 0.1450.02
Scaling of W for N jets? 4 jets
D0 Run II Preliminary
25
s(ttljets) Results (no m tag)
For s 7pb
26
s(ttljets) Event Selection (soft m tag)
  • Preselection criteria
  • Same as leptons jets except soft non-isolated
    muon is not vetoed
  • 3 jets with ETgt20 GeV hlt2.0
  • Aplanarity gt 0.04
  • HTgt110 GeV
  • Soft Muon Tag
  • pT(m)gt4 GeV within DRlt0.5 of a jet

For s 7pb
D0 Run II Preliminary
D0 Run II Preliminary
27
s(ttX) Cross Section
Combined
Combined
28
Conclusions
  • Four new W Z cross section measurements
  • Assuming same SM Z couplings to quarks and
    leptons, Z' is excluded at 95 CL at mZ'lt620 GeV
  • Combining the observation of the top decay
    channels an excess of 3s is observed, compatible
    with a signal expectation at the 35 CL

29
Backup Slides
30
Zee Candidate
31
W0mn Backgrounds
32
W0mn Efficiencies
  • Dimuon events
  • 1 m w/central track match
  • 1 Calorimeter m
  • Determine fraction of Calorimeter muons that meet
    local muon criteria

L1
L2
L3
33
Uncertainties
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