high mass drell yan differential cross-section (atlas)

6
High Mass Drell Yan Differential Cross-section (ATLAS) Paul Bell University of Geneva on behalf of the high mass DY analysis team 18/2/2013

Upload: herman-carter

Post on 30-Dec-2015

21 views

Category:

Documents


1 download

DESCRIPTION

High Mass Drell Yan Differential Cross-section (ATLAS). Paul Bell University of Geneva on behalf of the high mass DY analysis team 18 / 2 / 2013. The measurement. Measurement of DY differential cross section in di -electron channel As function of di -electron invariant mass - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: High Mass  Drell  Yan Differential Cross-section (ATLAS)

High Mass Drell Yan Differential Cross-section(ATLAS)

Paul BellUniversity of Geneva

on behalf of the high mass DY analysis team

18/2/2013

Page 2: High Mass  Drell  Yan Differential Cross-section (ATLAS)

The measurement Measurement of DY differential cross section in di-electron channel As function of di-electron invariant mass In “high mass” region = 116 – 1500 GeV Within “extended fiducial” region of electron pT > 25 GeV and | eta | < 2.5

CONF note: https://cds.cern.ch/record/1493623

(paper in approval)

Main backgrounds: W + jets & multijets where jet fakes the electron ID => data driven, 4 methods Other backgrounds from MC

2

Page 3: High Mass  Drell  Yan Differential Cross-section (ATLAS)

“Unfolding” method

Fiducial cross section within extended fiducial region given by

where CDY is the correction factor, given by

where NMC,reco = sum of MC signal events after simulation and selection in measured fiducial region (excludes the “crack” region)

NMC,gen-fid = sum of MC signal events at generator level within extended fiducial region

i.e. CDY includes the small extrapolation over the crack region.

Cross-section measured at different levels of QED FSR correction corresponding to different truth level definitions of NMC,gen-fid:

• Born level: Using electrons before QED FSR, i.e. full QED correction

• dressed level: Where 4-vectors of the bare lepton and all QED FSRphotons within a cone of ∆R < 0.1 are resummed

to perform a partial QED FSR correction3

Page 4: High Mass  Drell  Yan Differential Cross-section (ATLAS)

Results and systematics

4

Statistical uncertainty dominates for mee > 500 GeV

Reaches 50% in highest mee bin

Total systematic uncertainty within 10%

Dominated at low mee by electron efficiency and at high mee by background estimate

Page 5: High Mass  Drell  Yan Differential Cross-section (ATLAS)

Results: generator comparison

MC comparison at dressed level

MC predictions agree well in shape only, after scaling globally

5

Page 6: High Mass  Drell  Yan Differential Cross-section (ATLAS)

Results: FEWZ 3.1 comparison

FEWZ 3.1 comparisonat Born level with recent NNLO PDFs

FEWZ allows (N)NLO QCD corrections to be combined with the NLO electroweak corrections

Choice of EW scheme, Gµ or α(MZ), at most 0.4% effect, after applying NLO electroweak corrections

Contribution from photon-induced (PI) background, evaluated at LO using MRST2004qed

Correction from real W/Z radiation evaluated using MADGRAPH 5, at most 2% at highest mee (not shown) 6