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QCD with W/Z-events

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Run 1A: 20 pb-1 Run 1B: 80 pb-1 (Run 0- CDF: 4pb-1) 60k W-events, 5k Z-events /exp. ... M 80 GeV pT 5 GeV. M 91 GeV pT 6 GeV. measurements of d /dpT: ... – PowerPoint PPT presentation

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Title: QCD with W/Z-events


1
QCD with W/Z-events
  • Ursula Bassler, LPNHE-Paris
  • in behalf of the CDF and DØ collaborations
  • Basics on W/Z at the Tevatron
  • W/Z-production
  • Drell-Yan cross-section
  • d?/dPT for W and Z
  • W/Zjet production
  • W-decay
  • angular dependence of decay lepton
  • lepton charge asymmetry

2
Basics of W and Z production
  • W/Z production from qq annihilation
  • ?, pT distribution depend on pdf
  • large production
  • selection based on leptonic decays
  • W ? l? (BR 11 per mode)
  • ET(l) gt 25 GeV, ET(?) gt 25 GeV
  • Z ? ll (BR 3 per mode)
  • 2 isolated leptons, ET(l) gt 25 GeV
  • Run 1A 20 pb-1 Run 1B 80 pb-1
  • (Run 0- CDF 4pb-1)
  • ? 60k W-events, ? 5k Z-events /exp.

l
l
kinematic variables
3
Drell-Yan cross-section
  • access region at x gt 0.02 and up to Q2?15000
    GeV2
  • high mass Drell-Yan sensitivity to new physics
  • good agreement with NLO-calculation

4
Drell-Yan cross-section low mass
  • update of low mass Drell-Yan cross-section with
    reduced statistical errors
  • ee and ?? channel in good agreement
  • consistent with expected behavior

5
Drell-Yan at high rapidity
  • special analysis with leptons in the forward
    region
  • y1/2 ln x2/x1
  • access high x region
  • good agreement with gluon resummation calculation

6
pT dependence in W/Z-production
,W
q
q
q
,W
,W
q
q
q
  • O(?) W/Z bosons produced with pT0
  • pT attributed to gluon radiation, expected to
    broaden with Q2 M ? 10 GeV ??
    ltpTgt ? 1 GeV
  • M ? 80 GeV ? ltpTgt ? 5 GeV
  • M ? 91 GeV ?? ltpTgt ? 6 GeV
  • measurements of d?/dpT
  • W ? higher statistics, Z ? better resolution

7
Z-production at high pT
  • d?/dpT(Z) measured at 1 lt pT lt 230 GeV
  • cross-section falls over 5 orders of magnitude
  • perturbative QCD at O(?2) describes data at high
    pT

8
Z-production at low pT
  • at low pT soft gluon radiation dominates
  • resummation of large ln(Q2/pT2) terms
  • pT ?0 parameterize non-perturbative contribution
  • 2 formalisms possible
  • b-space resummation ? impact parameter space
  • qT-space resummation ? transverse momentum space

9
fit of Sudakov Form Factor
  • best description from
  • Ladinsky-Yuan
  • parameterization
  • fit to low mass Drell-Yan
  • and d?/dpT from CDF on
  • Run 0 data
  • non-perturbative Sudakov Form Factor
  • SNPLYg1b2g2b2ln(Q2/Q02)g1g3b ln(100xixj)
  • new fit of g20.590.06 GeV2 , reduced error
  • g1 and g3 in agreement with LY-value, similar
    error

10
pT dependence in W-production
  • d?/dpT(W) measured at 1 lt pT lt 180 GeV
  • error dominated by
  • low pT hadronic resolution
  • high pt statistics and backgrounds
  • good agreement with NNLO QCD low pt gluon
    resummation
  • DØ preliminary
  • MRSA - NNLOres.

11
W/Zjet production
  • hard gluon radiation produces additional jets
  • ?(W/Z ?1j)/?(W/Z)
  • depends on ?S
  • ?(W/Z ? Nj) in good agreement with
  • LO-calculation
  • soft scale ltpTgt2 favored

12
angular dependence in W-decay
?2
in W-rest frame
q
O(?)
sq
sq
sW
g
q
QCD
sq
sq
sW
13
charge asymmetry in W-decay
W
W-
u
d
  • constraints d/u ratio
  • measurement at Q2?M2W and 0.006 lt x lt 0.34
  • CDF combined e?
  • DØ ? only

14
Conclusions
  • W and Z bosons allow QCD studies using leptonic
    signatures, both in production and decay
  • Run II will start in march 2001
  • increased statistics (2 fb-1 / 2 years)
  • improved detectors
  • new and interesting results!
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