W Charge asymmetry

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W Charge asymmetry Cigdem Issever, Adam Scott, and David Stuart UCSB Preblessing, EWK 5/13/04 CDF Note 6282, Measurement of W e Charge Asymmetry CDF Note 6108, Alignment of the Plug Calorimeter CDF Note 6412, QCD Background for Plug Ws

description

W Charge asymmetry. Cigdem Issever, Adam Scott, and David Stuart UCSB. Preblessing, EWK 5/13/04. CDF Note 6282, Measurement of W  e n Charge Asymmetry CDF Note 6108, Alignment of the Plug Calorimeter CDF Note 6412, QCD Background for Plug Ws. Motivation. - PowerPoint PPT Presentation

Transcript of W Charge asymmetry

Page 1: W Charge asymmetry

W Charge asymmetry

Cigdem Issever, Adam Scott, and David Stuart

UCSB

Preblessing, EWK 5/13/04

•CDF Note 6282, Measurement of W e Charge Asymmetry

•CDF Note 6108, Alignment of the Plug Calorimeter

•CDF Note 6412, QCD Background for Plug Ws

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Motivation

W± charge asymmetry arises from u(x)/d(x) in proton.

Gives most sensitive u/d constraint at our x and Q2

But still not well constrained at high x (high . We don’t already know the answer.

Experimentally appealing.

Can improve many of our forthcoming measurements.

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Damn the ’s. forward e ahead

Asymmetry in W production complicated by unknown pz

So, use lepton asymmetry

Which convolves production asymmetry with V-A decay.

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Damn the ’s, forward e ahead

Forward electrons with charge id are the key.

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Two points and a curvature

define a unique helix:• Primary vertex• Shower Max cluster

• ET |C|

Attach hits using OI tracking

Select track with better 2/dof

Phoenix Tracking

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Phoenix Tracking

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Plug Alignment (CDF6108)

Align plug (actually PES) with COT tracks:

allow offsets in x,y,z and a rotation in phi

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Plug Alignment

Measure and correct, iteratively from largest to smallest

, x & y, Z

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Internal Alignment

Residual misalignments attributed to internal octant offsets

Fit for and radial shifts in each octant.

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Consistent internals between bpel08 and bpel09

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Residuals look good after alignment

We performed various validity and systematic checks

and found it to be robust with small systematics.

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Charge ID

Incorrectly identifying the charge dilutes the asymmetry.

We can correct for it if we know the rate, fQ # wrong / total

Atrue = Ameas / (1-2fQ)

So make fQ small and measure it.

MC predicts fQ ≈ 1%.

But MC doesn’t know about residual mis-alignments etc.

We must measure it in data and cannot assume any dependence.

Measured fQ() with Z e+e-

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Z Event Selection

Baseline electron selection with COT or PHX track. ET>25 GeV

PHX track is slightly non-standard to optimize fQ.

# hits >= 4

2 < 8

2 > 0.5

Seed Pull < 0.4

80<mee<100 and compare central Qtag

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Charge ID Measurement

Errors calculated with Bayesian prescription, CDF5894.

fQCOT fQ

Phx

CDFII Preliminary ∫Ldt=170/pb

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W Event Selection

Baseline electron selection w/ PHX track.

ET>25 GeV

Missing ET > 25 GeV

50 < MT < 100 GeV/c2

No other EMO with ET>25 GeV

to suppress QCD and DY

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Check kinematic distributions

Data

MC

CDFII Preliminary ∫Ldt=170/pb

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Check kinematic distributions

Data

MC

CDFII Preliminary ∫Ldt=170/pb

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Holy Phi

Data

MC

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Raw Asymmetry

CDFII Preliminary ∫Ldt=170/pb

Curve is just a fit to guide the eye.

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Raw Asymmetry

CDFII Preliminary ∫Ldt=170/pb

Curve is just a fit to guide the eye.

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BackgroundWe correct the asymmetry for backgrounds from:

• W e Asymmetric, measured from MC

• Z e+e-

Asymmetric, measured from MC

• QCD

Symmetric, measured from data CDF 6412.

Use Iso vs MET.

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QCD Background systematic

Check assumption of non-correlation

small systematic, as long as we don’t use the

PEM 3x3 2 or 5x9 cuts (they are correlated with Iso)

upper limit by about a factor of 2.

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QCD BackgroundQ

CD

fra

ctio

n

We use 0.5 ± 0.25. Becomes significant for >1.8

CDFII Preliminary ∫Ldt=170/pb

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Corrected Asymmetry

CDFII Preliminary ∫Ldt=170/pb

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Compare to COT when it is available

CDFII Preliminary ∫Ldt=170/pb

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Compare PDFs to data

CDFII Preliminary ∫Ldt=170/pb

CTEQ5L

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Overlay CTEQ3,4,5L, GRV98LO, MRST+d/uCTEQ3,4 to 5 have less d/u from Run1 asym. We keep pulling in Run2.

CDFII Preliminary ∫Ldt=170/pb

Compare PDFs to data

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CP checkCDFII Preliminary ∫Ldt=170/pb

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A(||)CDFII Preliminary ∫Ldt=170/pb

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A(||)

Compared to Run1 e+

FMU

CDFII Preliminary ∫Ldt=170/pb

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Getting more sensitivity to AW

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Getting more sensitivity to AW

25 < ET < 35

35 < ET < 45

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A() with 25 < ET < 35 GeV

CDFII Preliminary ∫Ldt=170/pb

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A(||) with 25 < ET < 35 GeV

CDFII Preliminary ∫Ldt=170/pb

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A() with 35 < ET < 45 GeVCDFII Preliminary ∫Ldt=170/pb

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A(||) with 35 < ET < 45 GeVCDFII Preliminary ∫Ldt=170/pb

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Conclusion

W asymmetry provides new PDF constraints.