ellie dobson university of oxford on behalf of atlas and the w z jets csc note group dis 2008 n.
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Ellie Dobson (University of Oxford) On behalf of ATLAS and the W/Z+Jets CSC note group DIS 2008. W/Z+Jets production studies in ATLAS. Why study W/Z+jet events? How do we see such events in ATLAS? Summary of current MC studies. Events. 10 fb  1. M eff. Why study W/Z+jets?.

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ellie dobson university of oxford on behalf of atlas and the w z jets csc note group dis 2008
Ellie Dobson

(University of Oxford)

On behalf of ATLAS and the W/Z+Jets CSC note group

DIS 2008

W/Z+Jets production studies in ATLAS

Why study W/Z+jet events?

  • How do we see such events in ATLAS?
  • Summary of current MC studies

Ellie Dobson

why study w z jets
Ellie Dobson

Events

10 fb1

Meff

Why study W/Z+jets?
  • Detector
  • Tests lepton reconstruction & MEt in multi jet environment
  • Precision tests of jet reconstruction algorithms and techniques
  • Standard model physics
  • Testing ground of pQCD
  • Testing LO/NLO predictions
  • Tests of BFKL logarithms
  • PDF studies

Beyond the standard model physics

  • Background to many BSM searches
  • Events must be well understood before we start looking for new physics!
w z jets production in atlas
Ellie DobsonW/Z+jets production in ATLAS

Hard jets

Zooming in…..

PDF1

g

u

Hard Scatter

Underlying event

(low pt hadronic recoil)

d

W

PDF2

Example of W+1jet production

W/Z

  • LHC will be a ‘W and Z factory’
  • Early running will produce ~1fb-1 of data:
  • ~20 million Ws, ~2 million Zs that can be seen (electron decay)
  • ~1/3 of these produced in association with jets….

Lepton

MET/second lepton

Health warning! Back of the envelope calculation

w z jets reconstruction in atlas
Ellie Dobson

Muon trigger used to write Z→μμ and W→μν events to disk

W/Z+jets reconstruction in ATLAS
  • Jets reconstructed in the calorimeters. Jets are built from calorimeter towers which are ‘H1 style’ calibrated to hadron level)

Muons reconstructed as a combination of a track in the inner detector and the muon spectrometer

Met and SumPt determined by summing over calorimeter cells.

Electrons reconstructed as a combination of a track in the inner detector and the energy deposit in the EM calorimeter

Electron trigger system used to write Z→ee and W→eν events to disk

current activities

Leptons (ID, efficiency, background)

  • Methods of background subtraction
  • Jets (reconstruction, algorithms, bjets)
  • Unfolding corrections
  • Evaluating uncertainties
Current activities
  • CSC (Computer Systems Commissioning) activity currently underway in ATLAS to produce public notes on performance and analysis
  • This talk summarises the activities of the W/Z+jets CSC note
  • The work in the W/Z inclusive CSC note is also relevant
  • Electronic and muonic decay channels have been studied
  • The focus at the moment is on understanding the detector: current activities include:

Put picture of first page of note here

Ellie Dobson

mc simulation and event selection
Ellie DobsonMC simulation and event selection

W/Z+jets sample (used for main analysis)

  • Matched Alpgen/Herwig samples (using LO PDF set CTEQ6LL), with generator level filter requiring 1 truth cone04 jet and 1(2) electrons/muons within fiducial requirements

Offline procedure (default)

Z EVENTS

  • Mass cuts
  • 2 leptons

W EVENTS

  • 1xMet
  • 1 lepton
  • BG and comparison samples
  • MC@NLO, Pythia and Alpgen W, Z, dijet and other background samples

LEPTON

  • Pt > 25/20/15GeV
  • Fiducial η cuts
  • Track matching
  • Inner detector track
  • Isolation cut from jets
  • Deposit of appropriate shape in calorimeter (electrons)
  • Hits in muon spectrometer (muons)

JET

  • Pt>20 or 40 GeV
  • Fiducial rapidity cuts
  • Isolation from leptons
  • Seeded cone 04 algorithm used

MET

  • Met>25GeV (W events)
correcting from parton hadron level
Ellie DobsonCorrecting from parton-hadron level
  • Data measurements compared to theory predictions at hadron level

→ need to correct theory with respect to fragmentation and underlying event

  • Determine corrections by comparing Pythia hadron level results with non perturbative effects switched on/off
  • Underlying event and fragmentation have the opposite effect
  • Precise behaviour depends on the jet algorithm used

Underlying event adds energy to the hadron level jet

Fragmentation reduces the amount of energy in the jet cone

Negligible effect for higher energy jets

trigger and reco efficiencies z ee
Ellie DobsonTrigger and reco efficiencies (Z→ee)
  • Single electron trigger (e25i) used to select Z → ee and W → eν events
  • e25i efficiency determined using a ‘tag and probe’ data driven method (although results shown are obviously ‘pseudo data’ for the time being….)
  • The numbers may be used to determine Z → ee or W → eν cross section
  • Sufficient in inclusive study to consider the efficiency as a function of η and pt only
  • In these more ‘jetty’ events is important to study the efficiency as a function of jet variables (distance to closest jet, hadronic activity, jet multiplicity….)
  • Global trigger efficiency ~1.5% lower than in the Pythia inclusive sample

Trigger efficiency

Reconstruction efficiency

Fall with higher hadronic

activity due to the implicit

isolation cut in the level 1 trigger

unfolding of detector effects z ee
Ellie DobsonUnfolding of detector effects (Z→ee)
  • Need to unfold data (jet and electron resolutions and reconstruction efficiencies) from detector level to hadron level
  • Will eventually determine jet resolution and efficiency from real data

Bias in reconstruction at low jet pt

No global behaviour seen

Within errors, the

Pt distributions of truth and

corrected reconstructed jets agree

bg estimation and subtraction z
BG estimation and subtraction (Z)
  • Z-ττ, ttbar and W → lνare, for now, estimated and subtracted using MC estimates
  • Weighting factors used for QCD due to the enormous cross section of this process
  • Fits may be used to estimate QCD backgrounds in real data
  • Can also derive this background by inverting selected electron ID cuts

Muons coming from background (particularly bbar) can be rejected using isolation requirements

QCD background dominates at a 1 jet signal. At higher jet multiplicity ttbar dominates.

Mass cuts imposed to reduce background

Ellie Dobson

slide11
Ellie Dobson

BG estimation and subtraction (W)

QCD

  • QCD largest background
  • ttbar dominates at high Njets
  • W→τν and Z →ee estimated using MC
  • Pythia underestimates QCD
  • QCD can be estimated from data using photon trigger and normalising to electron spectrum in sideband
  • QCD also can be estimated using fake rates

Zee

Weν

ttbar

W→τν

jet energy scale jes uncertainties
Ellie DobsonJet energy scale (JES) uncertainties
  • Dominant experimental systematic for W/Z+jets at the LHC
  • Miscalibration of ±1, 3, 5% assumed on the jet energy and effect on jet pt calculated
  • Main effect on the cross section results from the selection cut on the jet pt
  • Within early running (1fb-1) we hope to be within 3% JES uncertainty

→ systematic on the cross section of up to 10%

  • JES uncertainty of 1% (ultimate ATLAS goal) yields systematic of 0.5%

W events

Uncertainties increase with jet multiplicity

pdf uncertainty studies
Ellie DobsonPDF uncertainty studies
  • Must get these right or SM physics could be misinterpreted as new physics!
  • PDF uncertainties often the dominant theoretical uncertainty
  • PDF forms determined from combination of theoretical calculations and data
  • Free parameters of fit are given in a PDF set with their upper and lower errors
  • Overall PDF uncertainties calculated with PDF reweighting on NLO CTEQ6M set
  • PDF uncertainty ≤ JES uncertainty

Uncertainties always remain <10%

Shown results for W→eν.

Similar results seen in the muons and Z analysis

PDF errors increase at central η and at low electron Pt (no y dependence seen)

cross section results z ee
Ellie DobsonCross section results (Z→ee)
  • MCFM predictions corrected (for underlying event and fragmentation) to hadron level
  • Data unfolded to hadron level
  • PDF and JES uncertainties are included in the error determination
  • Cross sections quoted wrt inclusive to factor out luminosity uncertainty in early data

Pythia predicts a softer pt spectrum

Pythia discrepancies due to tuning of leading soft radiation in parton shower

slide15
Ellie Dobson

XS (Z →μμ)

  • Data unfolded to hadron level as before
  • Choice of isolation cone size must be optimised so to balance muon reconstruction efficiency and background rejection
  • Cross sections normalised to NLO
  • MCFM predictions corrected and compared to unfolded reconstructed events

Unfolded distribution

Pytha predicts more low pt jets

Pythia parton

shower predicts softer jet pt distribution

Alpgen predicts more high pt jets

z bjets
Ellie DobsonZ→μμ+bjets
  • A cross section measurement in this channel will provide an important test of pQCD
  • Will reduce the current uncertainty on the partonic heavy flavour content
  • This channel will be a lot easier at the LHC than at the Tevatron (higher production cross section, smaller background from Z+cjet)

btagging: cutting on the weight parameter (secondary vertex and impact parameter)

Contamination from light jets of the order 30%

conclusions
Ellie DobsonConclusions
  • W/Z+jets used as a standard candle to understand the detector
  • Understanding necessary in SM and BSM sectors
  • Specific findings:
    • Efficiencies ~1% lower than the inclusive due to hadronic isolation
    • Cuts developed so that signals are larger than background sum
    • Tools for estimating the dominant backgrounds from data developed
    • Two main non perturbative effects neglible above a jet Pt of 40GeV
    • Comparisons made between theory (corrected to the hadron level) and data (unfolded from detector level) are in agreement
    • JES dominant systematic. Will be reduced to ~3% after 2 years
    • This is larger than dominant theoretical uncertainty (PDF uncertainties)