a. nikitenko (ic/itep), rdms meeting, march.2009

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J J et et P P lus lus T T racks racks Sub-group of JetMET: Sub-group of JetMET: RDMS members: I. Vardanyan, N. RDMS members: I. Vardanyan, N. Ilina, Ilina, O. Kodolova, A. Nikitenko O. Kodolova, A. Nikitenko (convener) (convener) A. Nikitenko (IC/ITEP), RDMS meeting, March.2009 AN 2009-031, PAS JME-09-002

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J et P lus T racks Sub-group of JetMET: RDMS members: I. Vardanyan, N. Ilina, O. Kodolova, A. Nikitenko (convener). AN 2009-031, PAS JME-09-002. A. Nikitenko (IC/ITEP), RDMS meeting, March.2009. Jet+tracks algorithm. The goal of algorithm: correct calorimeter jet - PowerPoint PPT Presentation

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Page 1: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

JJet et PPlus lus TTracksracksSub-group of JetMET:Sub-group of JetMET:

RDMS members: I. Vardanyan, N. Ilina,RDMS members: I. Vardanyan, N. Ilina,O. Kodolova, A. Nikitenko (convener)O. Kodolova, A. Nikitenko (convener)

A. Nikitenko (IC/ITEP), RDMS meeting, March.2009

AN 2009-031, PAS JME-09-002

Page 2: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Jet+tracks algorithmJet+tracks algorithm

=0.5=0.5

The goal of algorithm: correct calorimeter jet energy to the energy of particles at vertex. out-of-calo-cone track in-calo-cone track

Basic algorithm steps:Basic algorithm steps:0. ZSP and PU off-set corr.0. ZSP and PU off-set corr.1.1. Subtract average expected Subtract average expected response of “in-calo-cone” response of “in-calo-cone” tracks from calo jet energy tracks from calo jet energy and add track momentum and add track momentum 2.2. Add momentum of “out-of-cone”Add momentum of “out-of-cone” trackstracks

Jet axis

Page 3: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Step 0: ZSP corrections

To be extracted from non ZSP data using single jet triggers

Page 4: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Step 1: correction for response of in-calo-cone tracks

EJet = EJetcalo – <Etrk

calo> + ptrk ,

<Etrkcalo> from data without ZSP

Page 5: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Response of pions from TB06Response of pions from TB06no zero suppressionno zero suppression

Page 6: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

In-calo-cone tracks corrections In-calo-cone tracks corrections with TB “jets”with TB “jets”

Jet was formed from chargedpions (-) randomly selected from the data. Number of pions in jet is fixed:

jet consists of 6 pions of 2 GeV4 pions of 3 GeV2 pion of 4 GeV1 pion of 5 GeV

thus true jet energy is 37 GeV

Average particle response(see previous slide) wassubtracted from jet raw energyand replaced by track momentum

Page 7: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Single particle response: effect of ZSP (MC study)

Input to JPT: non ZSP response of single pions

Effect of ZSP on single pion response

Page 8: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Step 2: adding out-of-calo-cone tracks

EJet = EJet+ ptrk (trks 1,2,3 in fig)

Page 9: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Steps 0-2 in one plot

Page 10: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Take into accountTake into account tracker inefficiency (I) tracker inefficiency (I)

Ein-cone = ntrkin-cone(pT

bin, bin) x (1-trk)/trk x (<pbin> - <Ecalo>)

Eout-of-cone = ntrkout-of-cone(pT

bin, bin) x (1-trk)/trk x <pbin>

trk = F(pTbin, bin) – track finding efficiency

Page 11: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Jet Energy Scale andJet Energy Scale and tracker inefficiency tracker inefficiency

Page 12: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

JES uncertainty due to single particle response

Page 13: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Performance for |Performance for ||<1.4|<1.4 Jet Enery Scale ET

reco / ETgen

Resolution:(ET

reco / ETgen)/(ET

reco / ETgen)

Page 14: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Performance for 1.4<|Performance for 1.4<||<2.0|<2.0 Jet Enery Scale ET

reco / ETgen

Resolution:(ET

reco / ETgen)/(ET

reco / ETgen)

Page 15: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Current JES vs Current JES vs

Still need to take intoaccount ECAL crystal calibration and more accurate response function

Page 16: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Calo vs Calo vs PF vs JPTPF vs JPT

Performance in CMSSW_2_2_3,full sim. after L2L3 corrections;“Official” JetMET plot

Latest PF improvements for 31Xvs JPT and calo in 2_2_3(see more in Michele’s talk)

Plot provided by P. Janot, no L2L3 corrections applied

ET >40 GeV, barrel

ET> 40 GeV, barrel

Page 17: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Work in progress to improve Work in progress to improve JPT for 31X releasesJPT for 31X releases

It was Monte-Carlo.It was Monte-Carlo.

Need time to commission JPT using Need time to commission JPT using real data: ZSP, single particle real data: ZSP, single particle

response, tracker efficiency from data; response, tracker efficiency from data;

Page 18: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

tcMETtcMET = MET(corrected for MET(corrected for )) – pp + 〈〈 EE 〉〉(Replacing expected calorimeter responseexpected calorimeter response with track momentumtrack momentum)

Frank Golf et al.

CMSSW_1_6_XCMSSW_1_6_XCMSSW_1_6_XCMSSW_1_6_X

# of evts with MET>30 GeV (in Z’s) faked by detector resolution and other effects: reduced by factor ~3, while # of W’s almost unaffected as expected.# of evts with MET>30 GeV (in Z’s) faked by detector resolution and other effects: reduced by factor ~3, while # of W’s almost unaffected as expected.

METtcMET

Missing Energy (GeV)

2.5)&GeV 20(

2)N(DY

T

p

Z/*

N(MET>30) ≈ 3 3 N(tcMET>30)

Case where we don’t expect MET …

2.5)&GeV 20(

1)N(T

p

W

Missing Energy (GeV)

N(MET>30) ≈ N(tcMET>30)

Case where we have true MET …

Track-corrected METTrack-corrected MET

Jan 19, 2009Meeting with LHCC referees

18

Page 19: A. Nikitenko (IC/ITEP), RDMS meeting,  March.2009

Performance for |Performance for ||<1.4|<1.4 Jet Enery Scale ET

reco / ETgen

Resolution:(ET

reco / ETgen)/(ET

reco / ETgen)

ZSP corrections: corrections for zero suppression on calo sells