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W/Z PRODUCTION AND PROPERTIES
Anton Kapliy (University of Chicago)on behalf of the ATLAS collaboration
PHENO-2012
2ATLAS measurements
2010 dataset
• Results shown in this talk use the 2010 dataset (~35 pb-1).• Work ongoing to update precision EWK measurements to the full 2011 dataset.
3W/Z cross-sections: why and how
• Precision tests of pQCD at NNLO• Sensitivity to Parton Distribution Functions (PDFs)• Clean signature: leptons and missing energy• 2010 dataset provides a rich sample of W’s and Z’s: – ~270k W candidates– ~24k Z candidates
• 2010 measurement has a total uncertainty on W and Z cross-sections on the order of a few percent.
• At NLO, variation of renormalization and factorization scales alone introduces a ~3% uncertainty on the theoretical predictions (down to ~0.5% at NNLO)
• FEWZ and DYNNLO programs are used with several NNLO PDF sets
4Monte-Carlo samples
Di-electron invariant mass W transverse mass (muon channel)
• In general, Monte-Carlo shows remarkable agreement with data.• It is corrected for pileup, reconstruction/identification efficiency, and
energy scale and resolution• Electroweak backgrounds are taken from MC; QCD is data-driven.
5Fiducial cross-sections• Electron and muon channels combined in common fiducial region• Include correlations between all three channels: W+, W-, Z• Cross-sections are also extrapolated to the full phase space:• This introduces a sizeable acceptance uncertainty
• Precision measurements are more sensitive in the fiducial region.
6Lepton universalityRatio of electron and muon cross-sections is performed in a common fiducial region.
Many uncertainties are correlated between electron and muon channels and cancel in the ratio:• Luminosity• Theory extrapolation
(acceptance)• Electroweak backgrounds• Pileup effects, etc
e-µ universality is confirmed in both W and Z ratios.
RW (ATLAS) World Average1.006±0.024 1.0017±0.019
RZ (ATLAS) World Average1.018±0.031 0.9991±0.0024
7Cross-section ratios
Some systematics (including luminosity uncertainty) cancel in the ratio of W±/Z and W+/W- cross-sections.
Overall, there is good agreement with NNLO predictions. We also see sensitivity to different PDF sets, especially in the W+ to W- ratio.
Differential cross-sections 8
Vector boson rapidity is sensitive to PDFs:
For W’s, it’s easier to work with lepton pseudorapidity (ηl).
Overall, there is good agreement with NNLO predictions, although there is tension with some PDF choices:• JR09 predicts lower Z cross-section at central rapidities• ABKM09 overshoots W cross-section at larger |ηl|
W charge asymmetry 9
Motivation:• Alternative probe of PDF structure• Sensitive to valence quarks at
Bjorken x ≈ 0.001 – 0.1• This region is not strongly
constrained by HERA.• Many systematics cancel!
Measurement:• Largely statistically limited• ABKM09 and HERAPDF give the
best agreement.• ATLAS+CMS+LHCb combination:• First useful PDF constraint from
LHC (→NNPDF2.2)
10Strange quark sea density
• Flavor SU(3) suggests the three light sea quark distributions are equal. This implies:
• Because strange is heavy, it may be suppressed– Current PDFs assume rs ≈ 0.5 at initial scale Q0
2=1.9 GeV2
• ATLAS measurements can improve this!– Parameterize qi(x) and g(x) at Q0
2=1.9 GeV2 (15 pars)– Perform NNLO fit to HERA DIS and ATLAS W+, W-, Z data– Unlike existing PDFs, don’t assume s(x)/d(x) ≈ 0.5 at Q0
2
• To visualize the results, rs is reported for existing and fitted PDFs at Q2=Q0
2 , x=0.023 and Q2=MZ2
, x=0.013
11Strange quark sea density: results
pQCD evolution
• Existing NNLO and NLO PDFs show tension with the new ATLAS prediction for strange quark density at Q2=1.9 GeV2
• Uncertainties are smaller at Q2=MZ2 because gluon splitting
probability is flavor independent, reducing any initial flavor asymmetries.• However, the same tension remains
12Incorporation of strange density results• As a consequence of enhanced strange quark density at low x, the
total light sea is enhanced by about 8% (left figure)• NNLO prediction for the ratio of W to Z cross-sections is in nearly
perfect agreement with data when using the PDFs that incorporate the new strange sea density results.
Total light sea with suppressed strange density (s/u fixed at 0.5), versus best-fit s/u = 1.0
13W polarization• W boson has 3 helicity states, with fractions fL, fR, f0 (longitudinal)• Different angular kinematics of W decay products → template fit
– cos(θ3D) – angle between W (lab frame) and lepton (W rest frame)
• To avoid neutrino pz ambiguity, we measure transverse cos(θ2D)– Unfolding to “full helicity” using Monte-Carlo information
• Separate measurements in two bins of pTW:
– pTW >50 GeV
– pTW =35..50 GeV
Definition of θ2D
J-B. Blanchard
14W polarization - resultsResults are averaged over lepton flavors and charges.Good agreement with theoretical predictions:• Low pT
W bin: compatible with both MC@NLO and POWHEG• Also cross-checked with Sherpa (not shown)
• High pTW bin: data favors somewhat lower values of f0
15W/Z + jets
• Precise tests of pQCD calculations and MC programs:– Novel Blackhat-Sherpa NNLO calculation– General-purpose Parton Shower (PS): Pythia– Matrix Element + Parton Shower (ME+PS): Alpgen, Sherpa
• Validation of detector performance and our understanding of a wide range of backgrounds
• Important irreducible background to new physics
Jet multiplicity 16
• Pythia predictions (PS) fail at high jet multiplicity• Alpgen (ME+PS) describes data well• Sherpa (ME+PS) has some tension with data• NLO calculation (Blackhat-Sherpa) is superbly accurate
W+jets Z+jets
Kinematic properties 17
• Well reproduced NLO and LO(ME+PS) predictions
pT of first jet, W+jets Dijet mass of two leading jets, Z+jets
18Conclusions
• Inclusive and differential measurements of W/Z cross-sections provide stringent tests for electroweak theory predictions
• Already with 2010 data, we are able to provide useful constraints for Parton Distribution Functions
• W/Z production in association with jets show remarkable agreement with NLO and LO (ME+PS) predictions for events with up to 4 jets.
• Much larger 2011 dataset will explore more differential distributions and substantially expand kinematic reach of the measurements.
BACKUP SLIDES
19
Inclusive cross-section values 20
Common fiducial region Extrapolation to total phase space
Inclusive cross-section systematics 21
Electron channel: Muon channel:
22W polarization
cos(θ3D) vs cos(θ2D) in MC:
Systematics for pTW>50 GeV bin
23W+jets: backgroundsUncorrected Njets distributions in muon and electron channels
24W/Z+jets: systematics
Jet energy scale systematic dominates for Njets > 0
Electron channel, at least one jet