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Karol Krizka and Michele Petteni



Simon Fraser University





CERN, 23/06/2009

Outline









Variable Definitions

Possible Backgrounds

Building Z → nunu Templates

Building Z → ll/W → lnu Templates









Karol and Michele (Simon Fraser University) Update 23/06/2009 2 / 28

Variable Definitons





− →



HT = PT + E T

TwoJets





−→

−− →



MHT = PT

TwoJets





−→ −

−− →

MET = ET









Note: For the vector variables, we plot the magnitude.



Karol and Michele (Simon Fraser University) Update 23/06/2009 3 / 28

Background Sources







Electroweak Background

Missing ET

Z → nunu

Unreconstructed Z → mumu and W → munu

Extra Jets and Missing ET

Z → ee

W → enu

QCD Backgrond









Karol and Michele (Simon Fraser University) Update 23/06/2009 4 / 28

Generator Level Cuts







Z → nunu has a generator level filter applied, so is inconsistent with the

other samples.

Filter:

Require at least one jet with

PT > 30 GeV

Eta 30GeV

Second Leading Jet ET > 30GeV

Third Leading Jet ET 100GeV

At least two reconstructed leptons (except Z → nunu)









Karol and Michele (Simon Fraser University) Update 23/06/2009 11 / 28

Missing ET









Karol and Michele (Simon Fraser University) Update 23/06/2009 12 / 28

Missing HT









Karol and Michele (Simon Fraser University) Update 23/06/2009 13 / 28

HT









Karol and Michele (Simon Fraser University) Update 23/06/2009 14 / 28

Building Z → ll / W → lnu Templates







Further assumptions:

There is no difference between reconstructed and non-reconstructed

Z’s.

There is no difference between non-reconstructed W’s and

reconstructed Z’s.

If these assumptions are true, we can combine all of the electroweak

background into one template.









Karol and Michele (Simon Fraser University) Update 23/06/2009 15 / 28

My Cuts









First Leading Jet ET > 30GeV

Second Leading Jet ET > 30GeV

Third Leading Jet ET 100GeV

No Reconstructed Leptons









Karol and Michele (Simon Fraser University) Update 23/06/2009 16 / 28

Background Cross Sections









Process Np0 Np1 Np2 Np3 Np4 Np5 Total

Z → nunu 0.000 1.318 18.291 8.461 2.042 0.305 30.42

Z → mumu 0.000 0.007 0.117 0.046 0.012 0.001 0.18

Z → ee 0.000 0.000 0.000 0.000 0.000 0.000 0.00

W → munu 0.003 0.546 6.639 2.941 0.719 0.106 10.95

W → enu 0.004 0.761 2.406 0.989 0.220 0.037 4.42









Karol and Michele (Simon Fraser University) Update 23/06/2009 17 / 28

Missing ET









Karol and Michele (Simon Fraser University) Update 23/06/2009 18 / 28

Missing HT









Karol and Michele (Simon Fraser University) Update 23/06/2009 19 / 28

HT









Karol and Michele (Simon Fraser University) Update 23/06/2009 20 / 28

Electron-Jet Contamination

It is possible that the electron in W → enu is detected as a jet, but not

reconstructed as an electron. This would drive missing ET down.

Solution:

Cut on the EM fraction of the two leading jets such that

0.1 < EM Fraction < 0.9









Karol and Michele (Simon Fraser University) Update 23/06/2009 21 / 28

W → enu Cut On EM Fraction, No MET Cut









Karol and Michele (Simon Fraser University) Update 23/06/2009 22 / 28

W → enu Cut On EM Fraction









Karol and Michele (Simon Fraser University) Update 23/06/2009 23 / 28

Detector Problems









It is possible that the difference between the reconstructed and

non-reconstructed plots could be due to kinematics that kept the leptons

from being reconstructed. For example, the muon chambers end at Eta of

about 2.6. Test:

Compare the truth ET of the reconstructed and non-reconstructed Z’s

Define a lepton as reconstructed if it lies within eta of 2.6









Karol and Michele (Simon Fraser University) Update 23/06/2009 24 / 28

Truth Z ET Distributions









Based on Monte Carlo

Karol and Michele (Simon Fraser University) Update 23/06/2009 25 / 28

Truth Z PT Distributions









Based on Monte Carlo

Karol and Michele (Simon Fraser University) Update 23/06/2009 26 / 28

Reconstructed Z → mumu Missing ET









Karol and Michele (Simon Fraser University) Update 23/06/2009 27 / 28

Detector Problems









The ET of the Z depends on eta and exhibits the same pattern as in

the reconstructed vs non-reconstructed missing ET plot

The PT of the Z depends on eta, but not as much as ET

We are currently modifying the missing ET of the event based on the

leptons’ ET . Maybe we should switch to PT ?









Karol and Michele (Simon Fraser University) Update 23/06/2009 28 / 28

Z → mumu Missing ET , Modified With Mu’s PT









Karol and Michele (Simon Fraser University) Update 23/06/2009 29 / 28



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