Top -> l+jets @ 10 TeV Updates on Efficiencies and Event Shapes
description
Transcript of Top -> l+jets @ 10 TeV Updates on Efficiencies and Event Shapes
Top -> l+jets @ 10 TeVUpdates on Efficiencies and Event
Shapes
Xiaowen Lei, Ken Johns, Venkat Kaushik
(U. Arizona)
Outline
Top with C++ ARA Redesign of code
Update on efficienciesUpdate on likelihood study
Analysis redone with bug-fixed Wjets sample; results look reasonable
TMVA approach
Started Muon Isolation Study
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Top with C++ ARAARATopAnalysis package developed by
Venkat is committed into the Arizona group cvs area
http://atlas-sw.cern.ch/cgi-bin/viewcvs-atlas.cgi/groups/Arizona/ARATopAnalysis/
ARATopAnalysis package provides the following Steering base class with common functions A default steering class with default selectors
Analysis in this talk was done by selection routines written by user (not the default ones)
Configuration and messaging service Scripts and executables for submitting jobs to
pandaAdditional details is available on twiki
https://twiki.cern.ch/twiki/bin/view/Sandbox/VKaushikSandbox#ARATopAnalysis
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ARATopAnalysis
Top with C++ ARASteering in ARATopAnalysis is used nowAnalysis methods are rewritten to separate
classes They serve as the user-implemented
“selectors” (processors)Helper classes for “communication”
between the processors are added. Selected objects are stored in
mySelectedObjects Event weights, trigger information, as well as
the cut bits are stored in myEventInfoRewrote the class for calculating
topological variables. Fixed some mistakes. Now it’s ready to be put into cvs
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Changes to the user analysis code
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EfficienciesLepton+jets selection efficiencies
were updated Weights are properly included Corrected W+jets samples are used
E368_s463_r563 Began processing smaller background samples
Updated samples include Wenu+Np: 108241, 108242, 108243; Wmunu+Np:
108245, 108246, 108247 Single top: 108240(schan_enu),
108241(schan_munu), 108243(tchan_enu), 108244(tchan_munu)
Tables are on the twiki page https://twiki.cern.ch/twiki/bin/viewauth/AtlasProtected/
TopCSBenchMark#Single_lepton_channel
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Cuts from the Spreadsheet Cut 1 – lepton trigger
EF_e20i or EF_mu20 Cut 2 – exactly 1 (medium) lepton with Pt>20GeV
For electron require isem(egammaPID::ElectronLoose) ==0 |eta|<2.5 && !(1.37<eta<1.52) etcone20<6GeV
For muon require |eta|<2.5 etcone20<6GeV
Note for muon, for the mc08 data, isolation is shifted down
etcone40 returns energy in cone with radius 0.3 should probably correct for it
Cut 3 – MET>20GeV Cut 4 – 4 good jets with Pt>30GeV Cut 5 – 3 good jets with Pt>40GeV Cut 6 – 150<m_jjj<190GeV
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e+jet Efficiencies
EfficienciesMC sample # Evt Cut 1 Cut 1-2 Cut 1-3 Cut 1-4 Cut 1-5 Cut 1-6
105200 55298 13861 9966 9016 2970 2558 611
105204
105205
105206 108396 29284 21348 18732 6510 5628 1460
108240
108241 23980 13018 10504 8820 111 78 11
108242 8500 4240 3420 2905 340 270 27
108243 3000 1357 1075 912 311 263 25
108340 10808 6186 5161 4561 73 68 8
108342
108343 2858 1505 1224 1091 37 28 2
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mu+jet Efficiency
Efficiencies
MC sample events cut 1 cut 1-2 cut 1-3 cut 1-4 cut 1-5 cut 1-6
105200 55298 14685 11850 10784 3745 3216 781
105204
105205
105206 108396 30428 24925 22124 7894 6820 1791
108244
108245 10500 5394 5250 4570 143 102 18
108246 6313 3193 3102 2708 496 385 52
108247 3000 1594 1543 1365 563 468 44
108341 11039 6243 6009 5382 58 45 7
108342
108344 8065 4516 4314 3855 150 115 16
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Topological Variables Analysis was redone with corrected W+jets
samples (e368_s462_r563) As a first step, used only 8242 (Np4) for Wenu+jets
and 8246(Np4) for Wmunu+jets Repeated our previous analysis to see if it works
No further optimization of the likelihood is done yet
Use events which passed cuts 1-5 A total number of 12 transformed variables are
currently used See following slides for plots of topological varialbes and
template functions
TMVA approach TMVA seems to be a good tool for optimizing the
likelihood
Topological Variables – mu+jetslog(ht):
sum(et) for jets et>15GeV
log(ht_2):log(et_j1+et_j2)
log(ht_3):log(et_j3+et_j4)
log(ht’_2):log(Sum(et)_j234/
Sum(pz)_j1234)
log(he) is also used but not shown here
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Topological Variables – mu+jets
log(centrality):log(ht/he)To remove?
exp(-11apla):apla = 3/2Q_1
log(sphe):sphe =
3/2(Q_1+Q_2)
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Topological Variables – mu+jetsLog(mjj_min):
minimum dijet mass
Use 4 leading jets
dPhi:angle between
leading lepton and missing et
log(K’_Tmin):minimum dijet
distance * et of the lower in the pair / hadronic W et
masschisq12
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Topological Variable Fits – mu+jets
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Topological Variable Fits – mu+jets
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Topological Variable Fits – mu+jets
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Topological Likelihood Lt
e+jets:
mu+jets:
Study with TMVA Get similar comparison plots and likelihood plots. TMVA
also give extra outputs which I am learning to understand TMVA is nice because it gives correlation between
variables. It can also be easily configured to use diferent variables
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Muon Isolation We started looking at muon isolation
As a first step we compared etcone20 (cone size 0.1) of ttbar (105200) and bbmu15X (108405)
No cuts on muons We are still at a very initial stage but plots can be
easily added and quickly produced A few things on our to-do list:
Compare etcone for different cone sizes. Also need to compare different inner cone sizes
Come up with cuts to extract the signal (muon from W)
Need to add cuts and change to log scale to see more clearly
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Conclusions Conclusions
We changed our C++ ARA code into a better design The code is ready to be put into cvs
We updated lepton+jets efficiency tables for bug-fixed W+jets samples and single-top samples
We redid our likelihood analysis with the new W+jets sample
Background still has low statistics We tried the same likelihood analysis with TMVA
Looked at the correlation matrix We made preliminary plots for muon isolation study
To-Do List To-do list:
We need to take into account the problem of shifted muon isolation
Since Atlfast samples for W+jets are available now (e368_a68), we can use them to increase the background statistics
Next we will consider single top as a background in our likelihood study
TMVA seems to be a nice tool for optimizing likelihood analysis. We want to use it to:
Try different combination of the variables Study the correlation between the variables
We would like to continue with muon isolation study
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