SUSY Jets + MET + Taus Analysis (2011 Data)
For the latest 2012 information, please see:
https://twiki.cern.ch/twiki/bin/view/Sandbox/SUSYJetsMETTausAnalysis2012
Motivation

[1]
%%mSUGRA%%
%\cite{msugra}
\bibitem{msugra}A. H. Chamseddine, R. L. Arnowitt, P. Nath, Phys. Rev. Lett. 49, 970 (1982); R. Barbieri,
S. Ferrara, C. A. Savoy, Phys. Lett. B119, 343 (1982); L. J. Hall, J. D. Lykken, S. Weinberg,
Phys. Rev. D27, 2359-2378 (1983); P. Nath, R. L. Arnowitt, A. H. Chamseddine, Nucl. Phys. B227, 121 (1983); For a review, see H. P. Nilles, Phys. Rept. 110, 1-162 (1984);
Stephen P. Martin, "A Supersymmetry Primer" [arXiv.hep-ph/9709356].

[2] R. Arnowitt et al., PRL 100, 231802 (2008) ... this is a paper to study
the signal of stau-neutralino co-annihilation at the LHC

[3] M.Dine and W. Fischler, Phys. Lett. B 110, 227 (1982);
C.R. Nappi and B.A. Ovrut, Phys. Lett. B 113, 175 (1982);
L. Alvarez-Gaum´e, M. Claudson and M.B. Wise, Nucl. Phys. B207, 96 (1982).

[4] E. Komatsu et al.,
ApJS, 192, 18 (2011) .... this is WMAP7 paper

I added Ref 3 for GMSB as another example of model with taus
to address one of Alfredo's suggestion of strengthening physics motivation.
120114_page1.jpg: Teruki's Comment's (01-14-2012)
Also see
http://faculty.physics.tamu.edu/kamon/research/refSUSY/
* tanB=10, A0 = 0
* tanB=40, A0 = -500
GeV (Yudi's mSUGRA)
(19-12-2011)
(17-01-2012)
Tasks in Preparation for 2012
(1) Upgrading
RA2Tau framework to work with 45X and 5X
(2) patTuples for 8
TeV MC
(3) QCD fake rates (tau ID commissioning)
(4) Tau ID in new running conditions
(5) How to measure tau ID scale factor with a ttbar control sample
(6)
SHyFT to measure tau ID scale factor vs. MHT/HT/Nvtx/Ztautau/W+Jets/ttbar/...
(7) Trigger efficiencies in MC vs. Jet Pt/MHT/HT/Nvtx/b-Tags/tau-Tags/...
SUS-12-004 Executive Summary of 2 jets + MHT + 2 taus
TTbar |
2.03 +/- 0.50 ("tau fake" method) |
(was 2.18 +/- 2.66 (stat+syst) at 1.1 fb-1) |
Wjets |
5.20 +/- 0.89 ("tau fake" method) |
(was 0.00 +/- 1.20 (stat+syst) at 1,1 fb-1) |
QCD |
0.02 +/- 0.02 |
(was 0.58 +/- 0.86 (stat+syst) at 1.1 fb-1) |
Znunu |
0.03 +/- 0.03 ("tau fake" method) |
(was 0.00 +/- 0.16 (stat+syst) at 1.1 fb-1) |
Ztautau |
0.21 +/- 0.20 ("tau fake" method) |
n.a. |
Total |
7.49 +/- 1.03 |
(was 2.76 at 1.1 fb-1) |
Data |
9 observed. |
(was 3 at 1.1 fb-1) |
* Q and A:
https://twiki.cern.ch/twiki/bin/view/Sandbox/SusyTauTauPaperAnswers2011
*
120307_mSUGRAlimitplot2.pdf: mSUGRA Excluded Region Distribution
*
120202_HtSignalPlot_m0280mhalf320.pdf: Data vs. MC HT Distribution
*
120202_MeffSignalPlot_m0280mhalf320.pdf: Data vs. MC Meff Distribution
* SM Cross-sections:
https://twiki.cern.ch/twiki/bin/viewauth/CMS/StandardModelCrossSections
SUS-12-004 (AN-11-519) & SUS-11-007 (AN-11-164) Milestones
Feb 24, 2012 |
Roy Montalvo |
Approval Talk |
TBA |
Feb 10, 2012 |
Roy Montalvo |
Pre-Approval Talk |
SUSY 3G Meeting http://roy.physics.tamu.edu/Work/PreApproval |
Feb 3, 2012 |
... |
AN and PAS, frozen |
... |
Jan 20, 2012 |
Roy Montalvo |
Status Report |
SUSY 3G Meeting |
Nov 6, 2011 |
Alfredo Gurrola |
SUS-11-007 Approval Talk |
SUSY General Meeting |
July 28, 2011 |
Andres Flrorez (RA2Tau); Matthias Edelhoff (RA6) |
SUS-11-007 Pre-Approval Talk |
SUSY General Meeting |
SUS-12-008 (AN-11-485) Milestones
* Use Higgs combination tool :
https://twiki.cern.ch/twiki/bin/viewauth/CMS/SWGuideHiggsAnalysisCombinedLimit
Filters
RA2 double-hadronic tau analysis (SUS-12-004) uses ALL filters,
but
RecovRecHitFilter:
Tools
We are using the
HighMassTau framework for skimming, patTuple creation, and analysis.
Installing & Running the Tools
Installation for 3_8_6
If you are working on FNAL machine, first prepare your environment:
source /uscmst1/prod/sw/cms/cshrc prod
In order to use the code, you need to create a CMSSW_3_8_6 working area:
scramv1 project CMSSW CMSSW_3_8_6
cd CMSSW_3_8_6/src
source /uscmst1/prod/grid/gLite_SL5.csh
cmsenv
source /uscmst1/prod/grid/CRAB/crab.csh
You will need to check out the High Mass Tau Group package. In order to do so, first log in to cvs as an anonymous user:
cmscvsroot CMSSW
cvs login
You will be prompted to enter a password. Use the following password: 98passwd
From cvs, checkout the High Mass Tau Group package:
cvs co -d HighMassAnalysis/Skimming -r for38x_PiZeros_HcalNoise UserCode/AlfredoGurrola/HighMassAnalysis/Skimming
cvs co -d HighMassAnalysis/Configuration -r for38x_PiZeros_HcalNoise UserCode/AlfredoGurrola/HighMassAnalysis/Configuration
cvs co -d HighMassAnalysis/Analysis -r forSusy_03092011_b UserCode/AlfredoGurrola/HighMassAnalysis/Analysis
cvs co -r V00-05-00 -d SHarper/HEEPAnalyzer UserCode/SHarper/HEEPAnalyzer
cvs co -r 1.25 RecoTauTag/tau_tags.txt
addpkg -f RecoTauTag/tau_tags.txt
Compile:
scram b -j8
Installation for 4_1_3
If you are working on FNAL machine, first prepare your environment:
source /uscmst1/prod/sw/cms/cshrc prod
In order to use the code, you need to create a CMSSW_4_1_3 working area:
setenv SCRAM_ARCH slc5_amd64_gcc434
scramv1 project CMSSW CMSSW_4_1_3
cd CMSSW_4_1_3/src
source /uscmst1/prod/grid/gLite_SL5.csh
cmsenv
source /uscmst1/prod/grid/CRAB/crab.csh
You will need to check out the High Mass Tau Group package as well as several other dependencies. In order to do so, first log in to cvs as an anonymous user:
cmscvsroot CMSSW
cvs login
You will be prompted to enter a password. Use the following password: 98passwd
Check out the Tags.csh script, which contains all the necessary dependencies that need to be checked out:
cvs co -d Tags -r 1.3 UserCode/AlfredoGurrola/HighMassAnalysis/Tags.csh
Next, run the Tags.csh script:
./Tags/Tags.csh
This will checkout all necessary packages and compile everything.
Installation for 4_2_4
If you are working on FNAL machine, first prepare your environment:
source /uscmst1/prod/sw/cms/cshrc prod
In order to use the code, you need to create a CMSSW_4_2_3 working area:
setenv SCRAM_ARCH slc5_amd64_gcc434
scramv1 project CMSSW CMSSW_4_2_4
cd CMSSW_4_2_4/src
source /uscmst1/prod/grid/gLite_SL5.csh
cmsenv
source /uscmst1/prod/grid/CRAB/crab.csh
You will need to check out the High Mass Tau Group package as well as several other dependencies. In order to do so, first log in to cvs as an anonymous user:
cmscvsroot CMSSW
cvs login
You will be prompted to enter a password. Use the following password: 98passwd
Check out the Tags.csh script, which contains all the necessary dependencies that need to be checked out:
cvs co -d Tags -r 1.18 UserCode/AlfredoGurrola/HighMassAnalysis/Tags.csh
Next, run the Tags.csh script:
./Tags/Tags.csh
This will checkout all necessary packages and compile everything.
Installation for 5_2_3_patch3
If you are working on FNAL machine, first prepare your environment:
source /uscmst1/prod/sw/cms/cshrc prod
In order to use the code, you need to create a CMSSW_5_2_3_patch3 working area:
setenv SCRAM_ARCH slc5_amd64_gcc462
scramv1 project CMSSW CMSSW_5_2_3_patch3
cd CMSSW_5_2_3_patch3/src
source /uscmst1/prod/grid/gLite_SL5.csh
cmsenv
source /uscmst1/prod/grid/CRAB/crab.csh
You will need to check out some specific packages. In order to do so, first log in to cvs as an anonymous user:
cmscvsroot CMSSW
cvs login
You will be prompted to enter a password. Use the following password: 98passwd
From cvs, checkout the following packages:
cvs co -r V00-03-07-01 CommonTools/ParticleFlow
cvs co -r V04-05-08 JetMETCorrections/Type1MET
cvs co -r CMSSW_5_2_3_patch3 PhysicsTools/CandUtils
cvs up -r 1.3 PhysicsTools/CandUtils/src/EventShapeVariables.cc
cvs co -r V08-08-25-01 PhysicsTools/PatAlgos
cvs co -r b5_2_X_cvMEtCorr_2012Apr10 PhysicsTools/PatUtils
cvs co -r CMSSW_5_2_3_patch3 RecoMET/METAlgorithms
cvs up -r 1.2 RecoMET/METAlgorithms/interface/SigInputObj.h
cvs co -r V15-01-05 RecoParticleFlow/PFProducer
cvs co -r V06-07-09 TopQuarkAnalysis/TopObjectResolutions
cvs co -d SHarper/HEEPAnalyzer UserCode/SHarper/HEEPAnalyzer
cvs co -r V01-04-17 RecoTauTag/RecoTau
cvs co -r V01-04-03 RecoTauTag/Configuration
cvs co -r V00-04-01 CondFormats/EgammaObjects
cvs up -r 1.53 PhysicsTools/PatAlgos/python/tools/tauTools.py
cvs up -r 1.12 PhysicsTools/PatAlgos/python/producersLayer1/tauProducer_cff.py
cvs up -r 1.15 PhysicsTools/PatAlgos/python/recoLayer0/tauDiscriminators_cff.py
cvs co -d HighMassAnalysis/Skimming -r for52x_05072012 UserCode/AlfredoGurrola/HighMassAnalysis/Skimming
cvs co -d HighMassAnalysis/Configuration -r for52x UserCode/AlfredoGurrola/HighMassAnalysis/Configuration
cvs co -d HighMassAnalysis/Analysis -r for52X_v4 UserCode/AlfredoGurrola/HighMassAnalysis/Analysis
Compile:
scram b -j8
Running Interactively: Testing PatTuple Producers
An example configuration file for creating patTuples exists in:
HighMassAnalysis/Configuration/test/Data_TauTauSkim/hiMassTau_patProd.py
The very first thing the user should check is that everything runs successfully interactively. To run a quick test, first make the following
modifications to hiMassTau_patProd.py :
1) Change the following lines:
process.maxEvents = cms.untracked.PSet(
input = cms.untracked.int32( 100 )
)
to the ones below:
process.maxEvents = cms.untracked.PSet(
input = cms.untracked.int32( 50 )
)
Changing 100 to 50 means that you will run over ONLY 50 events (-1 is for to run over all events). Next, open the file:
HighMassAnalysis/Configuration/python/hiMassSetup_cfi.py
This file only exists in pre 52X versions. In versions >= 52X, the parameters previously defined in hiMassSetup_cfi.py are defined in the
main configuration file, hiMassTau_patProd.py. This file defines the type of data sample that you want to create. If you want to run over a real collision data sample, then you MUST have the following variables defined:
signal = False
data = True
If you want to create patTuples beginning from a Monte Carlo RECO sample, then make the following definitions:
signal = False
data = False
NOTE: In the High Mass Tau group, we do NOT skim our signal samples. Therefore, If you do NOT want to skim a Monte Carlo sample,
set:
signal = True
This will ensure that no skimming criteria is applied. Finally, one must define the type of skimming.
1) Muon + Tau (loose mutau pair)
channel = "mutau"
2) Electron + Tau (loose etau pair)
channel = "etau"
3) Tau + Tau (loose ditau pair)
channel = "tautau"
4) Electron + Muon (loose emu pair)
channel = "emu"
5) Muon + Tau + Tau (loose ditau pair + muon)
channel = "mutautau"
6) Electron + Tau + Tau (loose ditau pair + electron)
channel = "electautau"
7)
SUSY (skim for collision data based on HLT_PFMHT150)
channel = "susy"
Once those modifications have been made, then you can test that everything works properly by running interactively:
cmsRun hiMassTau_patProd.py
Please look at all the output to make sure that no errors exist. Note that the default configuration file runs over a TTJets MC
sample located at FNAL. One might want to replace input
PoolSource to include the appropriate sample.
Creating PatTuples via CRAB and Writing out to Dcache
First, the user needs to verify that they indeed have a dcache area at FNAL:
ls /pnfs/cms/WAX/11/store/user/<USERNAME>
If your store/user area does not exist, please follow the instructions in the following link to request one:
http://www.uscms.org/uscms_at_work//software_computing/tier2/store_user.shtml
Alternatively, allowed users can write out to the
RA2Tau dcache area at FNAL:
ls /pnfs/cms/WAX/11/store/user/ra2tau
If the proper /store/user area exists, then create the following crab.cfg file:
[CRAB]
jobtype = cmssw
scheduler = condor
[CMSSW]
datasetpath = /ZPrime500TauTau_Tauola_GenSimRaw/eluiggi-ZPrime500TauTau_Tauola_GenSimReco-e775361b37e05a960708195f2a24a820/USER
dbs_url = http://cmsdbsprod.cern.ch/cms_dbs_ph_analysis_01/servlet/DBSServlet
use_parent = 0
pset = hiMassTau_patProd.py
total_number_of_events = -1
number_of_jobs = 50
output_file = skimPat.root
[USER]
ui_working_dir = SkimPat
return_data = 0
copy_data = 1
check_user_remote_dir = 0
storage_element = cmssrm.fnal.gov
storage_path = /srm/managerv2?SFN=/11
user_remote_dir=/store/user/<USERNAME>
publish_data = 1
publish_data_name = SkimPat
dbs_url_for_publication = https://cmsdbsprod.cern.ch:8443/cms_dbs_ph_analysis_01_writer/servlet/DBSServlet
srm_version = srmv2
#additional_input_files = Jec10V3.db
[GRID]
rb = CERN
proxy_server = fg-myproxy.fnal.gov
se_white_list =fnal
virtual_organization = cms
retry_count = 0
This configuration file is designed to create Monte Carlo patTuples. Make sure the appropriate USERNAME is replaced in the configuration above. NOTE: for versions >= 52X, the crab parameter
additional_input_files
is not needed and should be removed. To create your crab jobs:
crab -create -cfg crab.cfg
To submit your crab jobs:
crab -submit -c <CRAB_UI_NAME>
NOTE: The appropriate directory name must be substituted above.
To check the status of your jobs and retrieve the output:
crab -status -c <CRAB_UI_NAME>
crab -getoutput -c <CRAB_UI_NAME>
Notice that the above configuration is set up such that output files are published to DBS so that they may be accessed via CRAB
at a later time. To publish your dataset:
crab -publish -c <CRAB_UI_NAME>
How to use the Analysis Framework
Object Level Selections
How to apply pt > 15 and |eta|<2.1 cuts on hadronic taus?
RecoTauEtaCut = cms.double(2.1),
RecoTauPtMinCut = cms.double(15.),
RecoTauPtMaxCut = cms.double(9999.),
How to apply a leading track requirement on hadronic taus?
The pat::Tau object contains default "discriminators" that contain information about
whether a particular object passes the tau POG leading track/pion selections. In CMSSW_4_2_X,
the default leading track requirement is: leading tack pt > 5
GeV. The name of this discriminator
is "leadingTrackPtCut". Therefore, if the object contains a leading track with pt > 5
GeV, then
the value of "leadingTrackPtCut" is 1 ... If it fails this requirement, then the value is 0.
To apply a leading track requirement on hadronic taus:
DoRecoTauDiscrByLeadTrack = cms.bool(True),
The user can either use the defaul "leadingTrackPtCut" discriminator within the pat::Tau object, or
apply their own user defined leading track pt requirement. To use the default "leadingTrackPtCut"
discriminator, which requires leading track pt > 5, do the following:
UseRecoTauDiscrByLeadTrackFlag = cms.bool(True),
RecoTauDiscrByLeadTrack = cms.untracked.string('leadingTrackPtCut'),
If the user would like to apply their own user defined leading track pt cut, then:
UseRecoTauDiscrByLeadTrackFlag = cms.bool(False),
RecoTauLeadTrackThreshold = cms.double(7.0),
The above configuration will require the leading track of the tau to have pt > 7
GeV.
How to apply a decay mode requirement on hadronic taus?
The pat::Tau object contains default "discriminators" that contain information about
whether a particular object passes the tau POG decay mode selections. The default tau POG
decay mode finding requires a tau object to have 1 charged hadron with 0 "strips", or
1 charged hadron with 1 "strip", or 1 charged hadron with 2 "strips", or 3 charged hadrons
compatible with the tau mass (rho or a1 resonance).
How to apply isolation requirements on hadronic taus?
Event Level Selections
RECO Samples
38X Fall 10 RECO Samples
Here are the samples for 38X (
ProductionFall2010at7TeV):
Tau+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
SUSY LM2 |
0.6027 pb |
1 |
0.876595 +- 0.000701 |
TTBar |
149.6 pb |
1 |
0.975123 +- 0.000149 |
W+Jets |
29349 pb |
1 |
0.125999 +- 0.000085 |
ZInv+Jets |
4500 pb |
1 |
0.0.031478 +- 0.000118 |
DYtoTauTau |
1653 pb |
1 |
0.254495 +- 0.000304 |
QCDPt0to5 |
4.844e+10 pb |
1 |
0.000347 +- 0.000025 |
QCDPt5to15 |
3.675e+10 pb |
1 |
0.000676 +- 0.000020 |
QCDPt15to30 |
8.159e+08 pb |
1 |
0.034703 +- 0.000078 |
QCDPt30to50 |
5.312e+07 pb |
1 |
0.235186 +- 0.000235 |
QCDPt50to80 |
6.359e+06 pb |
1 |
0.542666 +- 0.000279 |
QCDPt80to120 |
7.843e+05 pb |
1 |
0.773755 +- 0.000234 |
QCDPt120to170 |
1.151e+05 pb |
1 |
0.888699 +- 0.000180 |
QCDPt170to300 |
2.426e+04 pb |
1 |
0.949111 +- 0.000122 |
QCDPt300to470 |
1.168e+03 pb |
1 |
0.984864 +- 0.000069 |
QCDPt470to600 |
7.022e+01 pb |
1 |
0.990986 +- 0.000067 |
QCDPt600to800 |
1.555e+01 pb |
1 |
0.992371 +- 0.000062 |
QCDPt800to1000 |
1.844e+00 pb |
1 |
0.993339 +- 0.000056 |
41X Spring 11 RECO Samples
Here are the samples for 38X (
ProductionSpring2011at7TeV):
Tau+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
SUSY LM2 |
0.6027 pb |
1 |
1.000000 +- 0.00000 |
TTBar |
149.6 pb |
1 |
0.969173 +- 0.000160 |
W+Jets |
29349 pb |
1 |
0.117855 +- 0.000083 |
DYToTauTau |
1653 pb |
1 |
0.239789 +- 0.000302 |
Zinv+Jets |
4500 pb |
1 |
0.032056 +- 0.000120 |
Muon+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
SUSY LM2 |
0.6027 pb |
1 |
1.000000 +- 0.00000 |
TTBar |
149.6 pb |
1 |
0.366092 +- 0.000446 |
W+Jets |
29349 pb |
1 |
0.048486 +- 0.000055 |
DYToTauTau |
1653 pb |
1 |
0.061911 +- 0.000171 |
Electron+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
SUSY LM2 |
0.6027 pb |
1 |
1.000000 +- 0.00000 |
TTBar |
149.6 pb |
1 |
0.653808 +- 0.000441 |
W+Jets |
29349 pb |
1 |
0.065717 +- 0.000064 |
42X Summer 11 RECO Samples
Tau+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
DYToTauTau |
1631 pb |
1 |
0.126620 +- 0.000234 |
QCD Pt-0to5 |
4.761652e+10 pb |
1 |
0.001028 +- 0.000031 |
QCD Pt-5to15 |
3.675e+10 pb |
1 |
0.001004 +- 0.000025 |
QCD Pt-15to30 |
8.159e+08 pb |
1 |
0.004568 +- 0.000020 |
QCD Pt-30to50 |
5.312e+07 pb |
1 |
0.097821 +- 0.000119 |
QCD Pt-50to80 |
6.359e+06 pb |
1 |
0.355775 +- 0.000189 |
QCD Pt-80to120 |
7.843e+05 pb |
1 |
0.608882 +- 0.000191 |
QCD Pt-120to170 |
1.151e+05 pb |
1 |
0.764597 +- 0.000172 |
QCD Pt-170to300 |
2.426e+04 pb |
1 |
0.866630 +- 0.000136 |
QCD Pt-300to470 |
1.168e+03 pb |
1 |
0.957101 +- 0.000082 |
QCD Pt-470to600 |
7.022e+01 pb |
1 |
0.985174 +/- 0.000061 |
QCD Pt-600to800 |
1.555e+01 pb |
1 |
0.990288 +- 0.000048 |
QCD Pt-800to1000 |
1.844e+00 pb |
1 |
0.992661 0.000043 |
QCD Pt-1000to1400 |
3.321e-01 pb |
1 |
0.994100 +- 0.000053 |
QCD Pt1400-1800 |
1.087e-02 pb |
1 |
0.995741 +- 0.000044 |
QCD Pt 1800 |
3.575e-04 pb |
1 |
0.996711 +- 0.000106 |
TTJets |
165 pb |
1 |
|
WJets |
31314 pb |
1 |
0.071361 +- 0.000037 |
Zinv+Jets |
4500 pb |
1 |
0.013753 +- 0.000079 |
Tau+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
TTBar |
|
1 |
0.946588 +- 0.000132 |
WJets |
|
1 |
0.071361 +- 0.000037 |
Muon+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
TTBar |
|
1 |
0.374379 +- 0.000258 |
DYToTauTau |
1653 pb |
1 |
0.066491 +- 0.000176 |
DYToMuMu |
1653 pb |
1 |
0.498022 +- 0.000345 |
WJets |
|
1 |
0.069013 +- 0.000038 |
Electron+Tau Skims
Sample |
Cross Section |
Filter Efficiency |
Skim Eff |
Tau+Tau Skims
/LM2_SUSY_sftsht_7TeV-pythia6/gurrola-LM2386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/TT_TuneZ2_7TeV-pythia6-tauola/gurrola-Ttbar386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/WJetsToLNu_TuneZ2_7TeV-madgraph-tauola/gurrola-Wjets386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/ZinvisibleJets_7TeV-madgraph/gurrola-ZinvJets386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/DYToTauTau_M-20_TuneZ2_7TeV-pythia6-tauola/gurrola-Ztautau386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_0to5_TuneZ2_7TeV_pythia6/gurrola-QCD0to5386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_5to15_TuneZ2_7TeV_pythia6/gurrola-QCD5to15386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_15to30_TuneZ2_7TeV_pythia6/gurrola-QCD15to30386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_30to50_TuneZ2_7TeV_pythia6/gurrola-QCD30to50386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_50to80_TuneZ2_7TeV_pythia6/gurrola-QCD50to80386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_80to120_TuneZ2_7TeV_pythia6/gurrola-QCD80to120386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_120to170_TuneZ2_7TeV_pythia6/gurrola-QCD120to170386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_170to300_TuneZ2_7TeV_pythia6/gurrola-QCD170to300386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_300to470_TuneZ2_7TeV_pythia6/gurrola-QCD300to470386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_470to600_TuneZ2_7TeV_pythia6/gurrola-QCD470to600386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_600to800_TuneZ2_7TeV_pythia6/gurrola-QCD600to800386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
/QCD_Pt_800to1000_TuneZ2_7TeV_pythia6/gurrola-QCD800to1000386TauTauSkimPat-7366c4ea4e829434dfceaf4d02b68f46/USER
Tau+Tau Skims
/LM2_SUSY_sftsht_7TeV-pythia6/florez-LM2413TauTauSkimPat-33b075c2d5f691949113a2658d7582f7/USER
/TTJets_TuneZ2_7TeV-madgraph-tauola/florez-Ttbar413TauTauSkimPat-6d7995e079abe1f0b04bb08efa8c4d1e/USER
/WJetsToLNu_TuneZ2_7TeV-madgraph-tauola/florez-Wjets413TauTauSkimPat-6d7995e079abe1f0b04bb08efa8c4d1e/USER
Muon+Tau Skims
/LM2_SUSY_sftsht_7TeV-pythia6/florez-LM2413TauTauSkimPat-33b075c2d5f691949113a2658d7582f7/USER
/TTJets_TuneZ2_7TeV-madgraph-tauola/florez-Ttbar413MuTauSkimPat-9798e5ab1d4a976e6f05eba49b220175/USER
/WJetsToLNu_TuneZ2_7TeV-madgraph-tauola/florez-Wjets413MuTauSkimPat-9798e5ab1d4a976e6f05eba49b220175/USER
/DYToTauTau_M-20_CT10_TuneZ2_7TeV-powheg-pythia-tauola/amarotta-Ztautau_mutauSkim_05242011-2279d553110ad6b57f0b67fd3faafef2/USER
/TTJets_TuneZ2_7TeV-madgraph-tauola/amarotta-TTBar_mutauSkim_06022011-2279d553110ad6b57f0b67fd3faafef2/USER
Electron+Tau Skims
/LM2_SUSY_sftsht_7TeV-pythia6/florez-LM2413TauTauSkimPat-33b075c2d5f691949113a2658d7582f7/USER
/TTJets_TuneZ2_7TeV-madgraph-tauola/florez-Ttbar413ETauSkimPat-bf245254503c42ca2911551e117c64fa/USER
/WJetsToLNu_TuneZ2_7TeV-madgraph-tauola/florez-Wjets413ETauSkimPat-bf245254503c42ca2911551e117c64fa/USER
Tau+Tau Skims
/DYToTauTau_M-20_TuneZ2_7TeV-pythia6-tauola/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-0to5_TuneZ2_7TeV_pythia6/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-5to15_TuneZ2_7TeV_pythia6/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-15to30_TuneZ2_7TeV_pythia6/grace-diTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-30to50_TuneZ2_7TeV_pythia6/grace-diTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
QCD Pt 50to80 (Not Publishable) /uscms_data/d2/rjmhrj/Samples/ForMB/SampleQCDpt50to80.log
/QCD_Pt-80to120_TuneZ2_7TeV_pythia6/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-120to170_TuneZ2_7TeV_pythia6/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-170to300_TuneZ2_7TeV_pythia6/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-300to470_TuneZ2_7TeV_pythia6/grace-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-470to600_TuneZ2_7TeV_pythia6/grace-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-600to800_TuneZ2_7TeV_pythia6/grace-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-800to1000_TuneZ2_7TeV_pythia6/rjmhrj-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-1000to1400_TuneZ2_7TeV_pythia6/grace-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-1400to1800_TuneZ2_7TeV_pythia6/grace-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/QCD_Pt-1800_TuneZ2_7TeV_pythia6/grace-DiTauSkim-75448fb324d0d74d73f257a7dc924fbf/USER
/TTJets_TuneZ2_7TeV-madgraph-tauola/gurrola-Ttbar424TauTauSkimPat-75448fb324d0d74d73f257a7dc924fbf/USER
/ZinvisibleJets_7TeV-madgraph/rjmhrj-DiTauPats-75448fb324d0d74d73f257a7dc924fbf/USER
Muon+Tau Skims
/TTJets_TuneZ2_7TeV-madgraph-tauola/amarotta-TTJets_mutauSkim_06222011-d2196243fc6117c733eff4717010f8b7/USER
/DYToMuMu_M-20_TuneZ2_7TeV-pythia6/gurrola-Zmumu424MuTauSkimPat-917b80447908505176b49c543284efa3/USER
/DYToTauTau_M-20_TuneZ2_7TeV-pythia6-tauola/florez-Ztautau_CMSSW424_MuTauSkimPat-d2196243fc6117c733eff4717010f8b7/USER
WJets is attached at the bottom of this page.
Electron+Tau Skims
2011 Collision Data Samples (SUSY Skim)
1.1ifb
/METBTag/rjmhrj-susy_skim-d98c0cbcf648486176475ae4204523aa/USER
/MET/rjmhrj-susy_skim-d98c0cbcf648486176475ae4204523aa/USER
4635 ipb
Published Datasets:
/METBTag/rjmhrj-lumi_mask_16004-178677-d98c0cbcf648486176475ae4204523aa/USER
/MET/rjmhrj-lumi_mask_16004-180252-e2e2ebe90bf5dc69c2027eb1b36e8eb5/USER
Files:
/uscms_data/d2/rjmhrj/Samples/ForMB/SampleAll2011Data.log
Samples for Validation of Tau ID
Runs: 160329 - 163869
Primary datasest: /TauPlusX/Run2011A-May10ReReco-v1/RECO
Pattuple: /TauPlusX/amarotta-TauPlusX_MuTauSkimMay10ReReco-v1_06212011-6f7bb896fd1f8364561c8ea9ef189621/USER
Runs: 165071 - 167175
Primary dataset: /TauPlusX/Run2011A-PromptReco-v4/RECO
Pattuple: /TauPlusX/amarotta-TauPlusX_MuTauSkimPromptReco-v4_06212011-6f7bb896fd1f8364561c8ea9ef189621/USER
All 2011 Data e-tau Skim
Parents:
/TauPlusX/Run2011A-May10ReReco-v1/RECO
/TauPlusX/Run2011A-PromptReco-v4/RECO
/TauPlusX/Run2011A-PromptReco-v5/RECO
/TauPlusX/Run2011A-PromptReco-v6/RECO
/TauPlusX/Run2011B-PromptReco-v1/RECO
Pattuple: /TauPlusX/rjmhrj-etau_16004-180252-93a3627cc60b21cd83c049a0fda21e1e/USER
2012 Collision Data Samples
* All 2012 Data mu-tau Skim
*
- 290 ipb - /TauPlusX/Run2012A-PromptReco-v1/RECO
/TauPlusX/willhf-TauPlusX_MuTauSkim_20042012-1eeb854a27f3fa5538d67dcba7455541/USER
- 400 ipb - /TauPlusX/Run2012A-PromptReco-v1/RECO
/TauPlusX/willhf-TauPlusX_MuTauSkim_400ipb_27042012-1eeb854a27f3fa5538d67dcba7455541/USER
*** TauPlusX/ ***
-Cert_190456-190688_8TeV_PromptReco_Collisions12_JSON.txt
/TauPlusX/gulerk-TauPlusX_MuTau_16042012-dafe88d41a814ab392d056eadf8d7251/USER
-Cert_190456-191276_8TeV_PromptReco_Collisions12_JSON.txt
/TauPlusX/gulerk-TauPlusX_MuTau_21042012-dafe88d41a814ab392d056eadf8d7251/USER
/WToMuNu_TuneZ2star_8TeV_pythia6/gulerk-WJets_MuTau_16042012-bde2a26de94facf2c0f3458b63d77317/USER
/DYToMuMu_M_20_TuneZ2star_8TeV_pythia6/gulerk-DYToMuMu_MuTau_16042012-bde2a26de94facf2c0f3458b63d77317/USER
/DYToTauTau_M-100to200_TuneZ2Star_8TeV-pythia6-tauola/gulerk-DYToTauTau_MuTau_16042012-bde2a26de94facf2c0f3458b63d77317/USER
Electron + Tau Triggers
For validation of tau ID, we will use the following un-prescaled cross-trigger:
HLT_Ele15_CaloIdVT_CaloIsoT_TrkIdT_TrkIsoT_LooseIsoPFTau15
Muon + Tau Triggers
For validation of tau ID, we will use the following un-prescaled cross-trigger:
HLT_IsoMu12_LooseIsoPFTau10
Samples for Final Analysis
Runs 160404-163869
/METBTag/Run2011A-May10ReReco-v1/RECO
Triggers
We will use the HLT_PFMHT150 trigger.
JSON File
Cert_160404-163869_7TeV_PromptReco_Collisions11_JSON.txt (Integrated Luminosity = 191.1 inverse pb)
Cert_160404-166502_7TeV_PromptReco_Collisions11_JSON.txt (Integrated Luminosity = 486 inverse pb)
Cert_160404-171116_7TeV_PromptReco_Collisions11_JSON.txt (Integrated Luminosity = 1092 inverse pb)
mSUGRA Scan
At the moment, these are the mSUGRA points that have sufficient statistics:
m0 = 360, m12 = 540, A0 = -500, sign(mu) > 0
m0 = 360, m12 = 560, A0 = -500, sign(mu) > 0
m0 = 400, m12 = 660, A0 = -500, sign(mu) > 0
m0 = 400, m12 = 680, A0 = -500, sign(mu) > 0
m0 = 420, m12 = 720, A0 = -500, sign(mu) > 0
m0 = 420, m12 = 740, A0 = -500, sign(mu) > 0
LM2 Generator Information (mSUGRA parameters, Masses, BRs)
The following mSUGRA parameters were used to generate the LM2 samples:
BLOCK MINPAR # Input parameters - minimal models
1 1.85000000E+02 # m0
2 3.50000000E+02 # m12
3 3.50000000E+01 # tanb
4 1.00000000E+00 # sign(mu)
5 0.00000000E+00 # A0
These are the masses at the EWK scale obtained using RGE's:
BLOCK MASS # Mass Spectrum
# PDG code mass particle
24 8.03895769E+01 # W+
25 1.12891876E+02 # h
35 4.33816133E+02 # H
36 4.33780276E+02 # A
37 4.41655229E+02 # H+
5 4.82427405E+00 # b-quark pole mass calculated from mb(mb)_Msbar
1000001 7.76942395E+02 # ~d_L
2000001 7.45684089E+02 # ~d_R
1000002 7.70205326E+02 # ~u_L
2000002 7.52189210E+02 # ~u_R
1000003 7.76942395E+02 # ~s_L
2000003 7.45684089E+02 # ~s_R
1000004 7.70205326E+02 # ~c_L
2000004 7.52189210E+02 # ~c_R
1000005 6.71211015E+02 # ~b_1
2000005 7.23970030E+02 # ~b_2
1000006 5.80036832E+02 # ~t_1
2000006 7.48044035E+02 # ~t_2
1000011 3.04110043E+02 # ~e_L
2000011 2.31071801E+02 # ~e_R
1000012 2.91957064E+02 # ~nu_eL
1000013 3.04110043E+02 # ~mu_L
2000013 2.31071801E+02 # ~mu_R
1000014 2.91957064E+02 # ~nu_muL
1000015 1.55702885E+02 # ~tau_1
2000015 3.14118803E+02 # ~tau_2
1000016 2.78934012E+02 # ~nu_tauL
1000021 8.26803768E+02 # ~g
1000022 1.40521545E+02 # ~chi_10
1000023 2.64266574E+02 # ~chi_20
1000025 -4.55433044E+02 # ~chi_30
1000035 4.68227895E+02 # ~chi_40
1000024 2.66559143E+02 # ~chi_1+
1000037 4.65210964E+02 # ~chi_2+
The following lists the
SUSY branching ratios:
# PDG Width
DECAY 1000021 7.11244132E+00 # gluino decays
# BR NDA ID1 ID2
1.62521059E-02 2 1000001 -1 # BR(~g -> ~d_L db)
1.62521059E-02 2 -1000001 1 # BR(~g -> ~d_L* d )
4.13558511E-02 2 2000001 -1 # BR(~g -> ~d_R db)
4.13558511E-02 2 -2000001 1 # BR(~g -> ~d_R* d )
2.07650818E-02 2 1000002 -2 # BR(~g -> ~u_L ub)
2.07650818E-02 2 -1000002 2 # BR(~g -> ~u_L* u )
3.52790965E-02 2 2000002 -2 # BR(~g -> ~u_R ub)
3.52790965E-02 2 -2000002 2 # BR(~g -> ~u_R* u )
1.62521059E-02 2 1000003 -3 # BR(~g -> ~s_L sb)
1.62521059E-02 2 -1000003 3 # BR(~g -> ~s_L* s )
4.13558511E-02 2 2000003 -3 # BR(~g -> ~s_R sb)
4.13558511E-02 2 -2000003 3 # BR(~g -> ~s_R* s )
2.07650818E-02 2 1000004 -4 # BR(~g -> ~c_L cb)
2.07650818E-02 2 -1000004 4 # BR(~g -> ~c_L* c )
3.52790965E-02 2 2000004 -4 # BR(~g -> ~c_R cb)
3.52790965E-02 2 -2000004 4 # BR(~g -> ~c_R* c )
1.30575560E-01 2 1000005 -5 # BR(~g -> ~b_1 bb)
1.30575560E-01 2 -1000005 5 # BR(~g -> ~b_1* b )
6.58812687E-02 2 2000005 -5 # BR(~g -> ~b_2 bb)
6.58812687E-02 2 -2000005 5 # BR(~g -> ~b_2* b )
7.62389008E-02 2 1000006 -6 # BR(~g -> ~t_1 tb)
7.62389008E-02 2 -1000006 6 # BR(~g -> ~t_1* t )
#
# PDG Width
DECAY 1000006 3.81921217E+00 # stop1 decays
# BR NDA ID1 ID2
2.08472268E-01 2 1000022 6 # BR(~t_1 -> ~chi_10 t )
1.51013561E-01 2 1000023 6 # BR(~t_1 -> ~chi_20 t )
4.67372616E-01 2 1000024 5 # BR(~t_1 -> ~chi_1+ b )
1.73141555E-01 2 1000037 5 # BR(~t_1 -> ~chi_2+ b )
#
# PDG Width
DECAY 2000006 1.06702138E+01 # stop2 decays
# BR NDA ID1 ID2
3.02372763E-02 2 1000022 6 # BR(~t_2 -> ~chi_10 t )
8.68255852E-02 2 1000023 6 # BR(~t_2 -> ~chi_20 t )
8.13259680E-02 2 1000025 6 # BR(~t_2 -> ~chi_30 t )
2.45430584E-01 2 1000035 6 # BR(~t_2 -> ~chi_40 t )
2.16291218E-01 2 1000024 5 # BR(~t_2 -> ~chi_1+ b )
2.26013883E-01 2 1000037 5 # BR(~t_2 -> ~chi_2+ b )
2.70588539E-02 2 1000006 25 # BR(~t_2 -> ~t_1 h )
8.68166313E-02 2 1000006 23 # BR(~t_2 -> ~t_1 Z )
#
# PDG Width
DECAY 1000005 5.42551095E+00 # sbottom1 decays
# BR NDA ID1 ID2
7.29582865E-02 2 1000022 5 # BR(~b_1 -> ~chi_10 b )
2.89932327E-01 2 1000023 5 # BR(~b_1 -> ~chi_20 b )
5.82837694E-02 2 1000025 5 # BR(~b_1 -> ~chi_30 b )
3.18648306E-02 2 1000035 5 # BR(~b_1 -> ~chi_40 b )
4.27935961E-01 2 -1000024 6 # BR(~b_1 -> ~chi_1- t )
1.10572626E-01 2 -1000037 6 # BR(~b_1 -> ~chi_2- t )
8.45219868E-03 2 1000006 -24 # BR(~b_1 -> ~t_1 W-)
#
# PDG Width
DECAY 2000005 5.63435797E+00 # sbottom2 decays
# BR NDA ID1 ID2
2.32574529E-02 2 1000022 5 # BR(~b_2 -> ~chi_10 b )
7.82936980E-02 2 1000023 5 # BR(~b_2 -> ~chi_20 b )
9.84448429E-02 2 1000025 5 # BR(~b_2 -> ~chi_30 b )
1.17153060E-01 2 1000035 5 # BR(~b_2 -> ~chi_40 b )
1.13875643E-01 2 -1000024 6 # BR(~b_2 -> ~chi_1- t )
4.65213054E-01 2 -1000037 6 # BR(~b_2 -> ~chi_2- t )
1.03762249E-01 2 1000006 -24 # BR(~b_2 -> ~t_1 W-)
#
# PDG Width
DECAY 1000002 7.29924898E+00 # sup_L decays
# BR NDA ID1 ID2
1.02718193E-02 2 1000022 2 # BR(~u_L -> ~chi_10 u)
3.15065941E-01 2 1000023 2 # BR(~u_L -> ~chi_20 u)
8.38072920E-04 2 1000025 2 # BR(~u_L -> ~chi_30 u)
1.38242469E-02 2 1000035 2 # BR(~u_L -> ~chi_40 u)
6.41499243E-01 2 1000024 1 # BR(~u_L -> ~chi_1+ d)
1.85006777E-02 2 1000037 1 # BR(~u_L -> ~chi_2+ d)
#
# PDG Width
DECAY 2000002 1.58306330E+00 # sup_R decays
# BR NDA ID1 ID2
9.91579744E-01 2 1000022 2 # BR(~u_R -> ~chi_10 u)
3.07561631E-03 2 1000023 2 # BR(~u_R -> ~chi_20 u)
1.21876699E-03 2 1000025 2 # BR(~u_R -> ~chi_30 u)
4.12587312E-03 2 1000035 2 # BR(~u_R -> ~chi_40 u)
#
# PDG Width
DECAY 1000001 7.19025984E+00 # sdown_L decays
# BR NDA ID1 ID2
1.81908754E-02 2 1000022 1 # BR(~d_L -> ~chi_10 d)
3.08682341E-01 2 1000023 1 # BR(~d_L -> ~chi_20 d)
1.45295693E-03 2 1000025 1 # BR(~d_L -> ~chi_30 d)
1.84619812E-02 2 1000035 1 # BR(~d_L -> ~chi_40 d)
6.02532850E-01 2 -1000024 2 # BR(~d_L -> ~chi_1- u)
5.06789952E-02 2 -1000037 2 # BR(~d_L -> ~chi_2- u)
#
# PDG Width
DECAY 2000001 3.92244471E-01 # sdown_R decays
# BR NDA ID1 ID2
9.91690601E-01 2 1000022 1 # BR(~d_R -> ~chi_10 d)
3.06535634E-03 2 1000023 1 # BR(~d_R -> ~chi_20 d)
1.19742954E-03 2 1000025 1 # BR(~d_R -> ~chi_30 d)
4.04661342E-03 2 1000035 1 # BR(~d_R -> ~chi_40 d)
#
# PDG Width
DECAY 1000004 7.29924898E+00 # scharm_L decays
# BR NDA ID1 ID2
1.02718193E-02 2 1000022 4 # BR(~c_L -> ~chi_10 c)
3.15065941E-01 2 1000023 4 # BR(~c_L -> ~chi_20 c)
8.38072920E-04 2 1000025 4 # BR(~c_L -> ~chi_30 c)
1.38242469E-02 2 1000035 4 # BR(~c_L -> ~chi_40 c)
6.41499243E-01 2 1000024 3 # BR(~c_L -> ~chi_1+ s)
1.85006777E-02 2 1000037 3 # BR(~c_L -> ~chi_2+ s)
#
# PDG Width
DECAY 2000004 1.58306330E+00 # scharm_R decays
# BR NDA ID1 ID2
9.91579744E-01 2 1000022 4 # BR(~c_R -> ~chi_10 c)
3.07561631E-03 2 1000023 4 # BR(~c_R -> ~chi_20 c)
1.21876699E-03 2 1000025 4 # BR(~c_R -> ~chi_30 c)
4.12587312E-03 2 1000035 4 # BR(~c_R -> ~chi_40 c)
#
# PDG Width
DECAY 1000003 7.19025984E+00 # sstrange_L decays
# BR NDA ID1 ID2
1.81908754E-02 2 1000022 3 # BR(~s_L -> ~chi_10 s)
3.08682341E-01 2 1000023 3 # BR(~s_L -> ~chi_20 s)
1.45295693E-03 2 1000025 3 # BR(~s_L -> ~chi_30 s)
1.84619812E-02 2 1000035 3 # BR(~s_L -> ~chi_40 s)
6.02532850E-01 2 -1000024 4 # BR(~s_L -> ~chi_1- c)
5.06789952E-02 2 -1000037 4 # BR(~s_L -> ~chi_2- c)
#
# PDG Width
DECAY 2000003 3.92244471E-01 # sstrange_R decays
# BR NDA ID1 ID2
9.91690601E-01 2 1000022 3 # BR(~s_R -> ~chi_10 s)
3.06535634E-03 2 1000023 3 # BR(~s_R -> ~chi_20 s)
1.19742954E-03 2 1000025 3 # BR(~s_R -> ~chi_30 s)
4.04661342E-03 2 1000035 3 # BR(~s_R -> ~chi_40 s)
#
# PDG Width
DECAY 1000011 4.10126636E-01 # selectron_L decays
# BR NDA ID1 ID2
5.35444761E-01 2 1000022 11 # BR(~e_L -> ~chi_10 e-)
1.78789777E-01 2 1000023 11 # BR(~e_L -> ~chi_20 e-)
2.85765462E-01 2 -1000024 12 # BR(~e_L -> ~chi_1- nu_e)
#
# PDG Width
DECAY 2000011 4.70202730E-01 # selectron_R decays
# BR NDA ID1 ID2
1.00000000E+00 2 1000022 11 # BR(~e_R -> ~chi_10 e-)
#
# PDG Width
DECAY 1000013 4.10126636E-01 # smuon_L decays
# BR NDA ID1 ID2
5.35444761E-01 2 1000022 13 # BR(~mu_L -> ~chi_10 mu-)
1.78789777E-01 2 1000023 13 # BR(~mu_L -> ~chi_20 mu-)
2.85765462E-01 2 -1000024 14 # BR(~mu_L -> ~chi_1- nu_mu)
#
# PDG Width
DECAY 2000013 4.70202730E-01 # smuon_R decays
# BR NDA ID1 ID2
1.00000000E+00 2 1000022 13 # BR(~mu_R -> ~chi_10 mu-)
#
# PDG Width
DECAY 1000015 2.51818300E-02 # stau_1 decays
# BR NDA ID1 ID2
1.00000000E+00 2 1000022 15 # BR(~tau_1 -> ~chi_10 tau-)
#
# PDG Width
DECAY 2000015 1.05907791E+00 # stau_2 decays
# BR NDA ID1 ID2
3.33390992E-01 2 1000022 15 # BR(~tau_2 -> ~chi_10 tau-)
7.05907664E-02 2 1000023 15 # BR(~tau_2 -> ~chi_20 tau-)
1.08010535E-01 2 -1000024 16 # BR(~tau_2 -> ~chi_1- nu_tau)
1.65740536E-01 2 1000015 25 # BR(~tau_2 -> ~tau_1 h)
3.22267170E-01 2 1000015 23 # BR(~tau_2 -> ~tau_1 Z)
#
# PDG Width
DECAY 1000012 3.38016867E-01 # snu_eL decays
# BR NDA ID1 ID2
7.13809368E-01 2 1000022 12 # BR(~nu_eL -> ~chi_10 nu_e)
9.83884019E-02 2 1000023 12 # BR(~nu_eL -> ~chi_20 nu_e)
1.87802231E-01 2 1000024 11 # BR(~nu_eL -> ~chi_1+ e-)
#
# PDG Width
DECAY 1000014 3.38016867E-01 # snu_muL decays
# BR NDA ID1 ID2
7.13809368E-01 2 1000022 14 # BR(~nu_muL -> ~chi_10 nu_mu)
9.83884019E-02 2 1000023 14 # BR(~nu_muL -> ~chi_20 nu_mu)
1.87802231E-01 2 1000024 13 # BR(~nu_muL -> ~chi_1+ mu-)
#
# PDG Width
DECAY 1000016 5.93863492E-01 # snu_tauL decays
# BR NDA ID1 ID2
3.66120536E-01 2 1000022 16 # BR(~nu_tauL -> ~chi_10 nu_tau)
1.71837130E-02 2 1000023 16 # BR(~nu_tauL -> ~chi_20 nu_tau)
2.70651794E-02 2 1000024 15 # BR(~nu_tauL -> ~chi_1+ tau-)
5.89630572E-01 2 -1000015 -24 # BR(~nu_tauL -> ~tau_1+ W-)
#
# PDG Width
DECAY 1000024 1.76407473E-01 # chargino1+ decays
# BR NDA ID1 ID2
9.47304925E-01 2 -1000015 16 # BR(~chi_1+ -> ~tau_1+ nu_tau)
5.26950754E-02 2 1000022 24 # BR(~chi_1+ -> ~chi_10 W+)
#
# PDG Width
DECAY 1000037 2.85010109E+00 # chargino2+ decays
# BR NDA ID1 ID2
1.23833484E-02 2 1000012 -11 # BR(~chi_2+ -> ~nu_eL e+ )
1.23833484E-02 2 1000014 -13 # BR(~chi_2+ -> ~nu_muL mu+ )
9.25832382E-02 2 1000016 -15 # BR(~chi_2+ -> ~nu_tau1 tau+)
2.90649344E-02 2 -1000011 12 # BR(~chi_2+ -> ~e_L+ nu_e)
2.90649344E-02 2 -1000013 14 # BR(~chi_2+ -> ~mu_L+ nu_mu)
5.67216914E-02 2 -1000015 16 # BR(~chi_2+ -> ~tau_1+ nu_tau)
6.23434334E-02 2 -2000015 16 # BR(~chi_2+ -> ~tau_2+ nu_tau)
2.09236846E-01 2 1000024 23 # BR(~chi_2+ -> ~chi_1+ Z )
8.12975927E-02 2 1000022 24 # BR(~chi_2+ -> ~chi_10 W+)
2.42802011E-01 2 1000023 24 # BR(~chi_2+ -> ~chi_20 W+)
1.72118622E-01 2 1000024 25 # BR(~chi_2+ -> ~chi_1+ h )
#
# PDG Width
DECAY 1000022 0.00000000E+00 # neutralino1 decays
#
# PDG Width
DECAY 1000023 1.84140363E-01 # neutralino2 decays
# BR NDA ID1 ID2
8.57115429E-03 2 1000022 23 # BR(~chi_20 -> ~chi_10 Z )
3.27939711E-02 2 1000022 25 # BR(~chi_20 -> ~chi_10 h )
7.51802968E-04 2 2000011 -11 # BR(~chi_20 -> ~e_R- e+)
7.51802968E-04 2 -2000011 11 # BR(~chi_20 -> ~e_R+ e-)
7.51802968E-04 2 2000013 -13 # BR(~chi_20 -> ~mu_R- mu+)
7.51802968E-04 2 -2000013 13 # BR(~chi_20 -> ~mu_R+ mu-)
4.77813831E-01 2 1000015 -15 # BR(~chi_20 -> ~tau_1- tau+)
4.77813831E-01 2 -1000015 15 # BR(~chi_20 -> ~tau_1+ tau-)
#
# PDG Width
DECAY 1000025 2.72577451E+00 # neutralino3 decays
# BR NDA ID1 ID2
9.12401998E-02 2 1000022 23 # BR(~chi_30 -> ~chi_10 Z )
1.90095662E-01 2 1000023 23 # BR(~chi_30 -> ~chi_20 Z )
2.28425319E-01 2 1000024 -24 # BR(~chi_30 -> ~chi_1+ W-)
2.28425319E-01 2 -1000024 24 # BR(~chi_30 -> ~chi_1- W+)
1.94836633E-02 2 1000022 25 # BR(~chi_30 -> ~chi_10 h )
8.78546567E-03 2 1000023 25 # BR(~chi_30 -> ~chi_20 h )
2.31122680E-04 2 1000011 -11 # BR(~chi_30 -> ~e_L- e+)
2.31122680E-04 2 -1000011 11 # BR(~chi_30 -> ~e_L+ e-)
6.27904981E-04 2 2000011 -11 # BR(~chi_30 -> ~e_R- e+)
6.27904981E-04 2 -2000011 11 # BR(~chi_30 -> ~e_R+ e-)
2.31122680E-04 2 1000013 -13 # BR(~chi_30 -> ~mu_L- mu+)
2.31122680E-04 2 -1000013 13 # BR(~chi_30 -> ~mu_L+ mu-)
6.27904981E-04 2 2000013 -13 # BR(~chi_30 -> ~mu_R- mu+)
6.27904981E-04 2 -2000013 13 # BR(~chi_30 -> ~mu_R+ mu-)
7.51865608E-02 2 1000015 -15 # BR(~chi_30 -> ~tau_1- tau+)
7.51865608E-02 2 -1000015 15 # BR(~chi_30 -> ~tau_1+ tau-)
3.58084543E-02 2 2000015 -15 # BR(~chi_30 -> ~tau_2- tau+)
3.58084543E-02 2 -2000015 15 # BR(~chi_30 -> ~tau_2+ tau-)
1.29874908E-03 2 1000012 -12 # BR(~chi_30 -> ~nu_eL nu_eb)
1.29874908E-03 2 -1000012 12 # BR(~chi_30 -> ~nu_eL* nu_e )
1.29874908E-03 2 1000014 -14 # BR(~chi_30 -> ~nu_muL nu_mub)
1.29874908E-03 2 -1000014 14 # BR(~chi_30 -> ~nu_muL* nu_mu )
1.46161735E-03 2 1000016 -16 # BR(~chi_30 -> ~nu_tau1 nu_taub)
1.46161735E-03 2 -1000016 16 # BR(~chi_30 -> ~nu_tau1* nu_tau )
#
# PDG Width
DECAY 1000035 3.06794452E+00 # neutralino4 decays
# BR NDA ID1 ID2
2.08649774E-02 2 1000022 23 # BR(~chi_40 -> ~chi_10 Z )
1.58692891E-02 2 1000023 23 # BR(~chi_40 -> ~chi_20 Z )
2.26992568E-01 2 1000024 -24 # BR(~chi_40 -> ~chi_1+ W-)
2.26992568E-01 2 -1000024 24 # BR(~chi_40 -> ~chi_1- W+)
6.79370114E-02 2 1000022 25 # BR(~chi_40 -> ~chi_10 h )
1.48843191E-01 2 1000023 25 # BR(~chi_40 -> ~chi_20 h )
6.01274602E-03 2 1000011 -11 # BR(~chi_40 -> ~e_L- e+)
6.01274602E-03 2 -1000011 11 # BR(~chi_40 -> ~e_L+ e-)
2.14301947E-03 2 2000011 -11 # BR(~chi_40 -> ~e_R- e+)
2.14301947E-03 2 -2000011 11 # BR(~chi_40 -> ~e_R+ e-)
6.01274602E-03 2 1000013 -13 # BR(~chi_40 -> ~mu_L- mu+)
6.01274602E-03 2 -1000013 13 # BR(~chi_40 -> ~mu_L+ mu-)
2.14301947E-03 2 2000013 -13 # BR(~chi_40 -> ~mu_R- mu+)
2.14301947E-03 2 -2000013 13 # BR(~chi_40 -> ~mu_R+ mu-)
4.04352982E-02 2 1000015 -15 # BR(~chi_40 -> ~tau_1- tau+)
4.04352982E-02 2 -1000015 15 # BR(~chi_40 -> ~tau_1+ tau-)
4.51253943E-02 2 2000015 -15 # BR(~chi_40 -> ~tau_2- tau+)
4.51253943E-02 2 -2000015 15 # BR(~chi_40 -> ~tau_2+ tau-)
1.42509047E-02 2 1000012 -12 # BR(~chi_40 -> ~nu_eL nu_eb)
1.42509047E-02 2 -1000012 12 # BR(~chi_40 -> ~nu_eL* nu_e )
1.42509047E-02 2 1000014 -14 # BR(~chi_40 -> ~nu_muL nu_mub)
1.42509047E-02 2 -1000014 14 # BR(~chi_40 -> ~nu_muL* nu_mu )
1.58761646E-02 2 1000016 -16 # BR(~chi_40 -> ~nu_tau1 nu_taub)
1.58761646E-02 2 -1000016 16 # BR(~chi_40 -> ~nu_tau1* nu_tau )
#
# PDG Width
DECAY 26 3.59143946E-03 # h decays
# BR NDA ID1 ID2
7.83825152E-01 2 5 -5 # BR(h -> b bb )
7.38232702E-02 2 -15 15 # BR(h -> tau+ tau- )
2.61378621E-04 2 -13 13 # BR(h -> mu+ mu- )
5.64967627E-04 2 3 -3 # BR(h -> s sb )
2.17132254E-02 2 4 -4 # BR(h -> c cb )
5.78274129E-02 2 21 21 # BR(h -> g g )
1.76657643E-03 2 22 22 # BR(h -> gam gam )
4.68133068E-04 2 22 23 # BR(h -> Z gam )
5.44494786E-02 2 24 -24 # BR(h -> W+ W- )
5.30040552E-03 2 23 23 # BR(h -> Z Z )
#
# PDG Width
DECAY 35 7.49639384E+00 # H decays
# BR NDA ID1 ID2
8.52777982E-01 2 5 -5 # BR(H -> b bb )
1.41197243E-01 2 -15 15 # BR(H -> tau+ tau- )
4.99232557E-04 2 -13 13 # BR(H -> mu+ mu- )
8.19396226E-04 2 3 -3 # BR(H -> s sb )
2.99824721E-08 2 4 -4 # BR(H -> c cb )
9.39602170E-04 2 6 -6 # BR(H -> t tb )
3.72119672E-04 2 21 21 # BR(H -> g g )
4.04212803E-07 2 22 22 # BR(H -> gam gam )
8.54537445E-08 2 23 22 # BR(H -> Z gam )
1.05430529E-05 2 24 -24 # BR(H -> W+ W- )
4.97300309E-06 2 23 23 # BR(H -> Z Z )
4.07007674E-05 2 25 25 # BR(H -> h h )
3.19911805E-22 2 36 36 # BR(H -> A A )
5.60960867E-19 2 23 36 # BR(H -> Z A )
8.67940204E-04 2 1000022 1000022 # BR(H -> ~chi_10 ~chi_10)
1.38048472E-06 2 1000022 1000023 # BR(H -> ~chi_10 ~chi_20)
2.46836699E-03 2 1000015 -1000015 # BR(H -> ~tau_1- ~tau_1+)
#
# PDG Width
DECAY 36 7.46645543E+00 # A decays
# BR NDA ID1 ID2
8.52935700E-01 2 5 -5 # BR(A -> b bb )
1.41777441E-01 2 -15 15 # BR(A -> tau+ tau- )
5.01250447E-04 2 -13 13 # BR(A -> mu+ mu- )
8.22767193E-04 2 3 -3 # BR(A -> s sb )
2.67622120E-08 2 4 -4 # BR(A -> c cb )
2.02154992E-03 2 6 -6 # BR(A -> t tb )
3.55804365E-04 2 21 21 # BR(A -> g g )
4.78867995E-07 2 22 22 # BR(A -> gam gam )
6.55663438E-08 2 23 22 # BR(A -> Z gam )
8.89554461E-06 2 23 25 # BR(A -> Z h )
1.56551961E-03 2 1000022 1000022 # BR(A -> ~chi_10 ~chi_10)
1.05000722E-05 2 1000022 1000023 # BR(A -> ~chi_10 ~chi_20)
#
# PDG Width
DECAY 37 7.83084956E+00 # H+ decays
# BR NDA ID1 ID2
1.58809973E-03 2 4 -5 # BR(H+ -> c bb )
1.37634345E-01 2 -15 16 # BR(H+ -> tau+ nu_tau )
4.86602064E-04 2 -13 14 # BR(H+ -> mu+ nu_mu )
1.01633937E-05 2 2 -5 # BR(H+ -> u bb )
3.78179209E-05 2 2 -3 # BR(H+ -> u sb )
7.77844697E-04 2 4 -3 # BR(H+ -> c sb )
8.54012355E-01 2 6 -5 # BR(H+ -> t bb )
9.42966142E-06 2 24 25 # BR(H+ -> W+ h )
4.98307746E-09 2 24 36 # BR(H+ -> W+ A )
5.44333707E-03 2 1000024 1000022 # BR(H+ -> ~chi_1+ ~chi_10)
Endpoint Caculation
Endpoint: M
ττ = 91.9644
GeV
Results for 2X
Table of Efficiencies
An output cut flow table is generated once the job has finished running:
Filter Statistics for SusyAnalyzer-FilterStatisticsService
number of events processed = 1000, of which 27 passed all Filters
Cut Passed cumul. Efficiency Efficiency excl. Rejection
--------------------------------------------------------------------------------------------------------------------------------------
>= 1 jet not overlaped w/ taus 1000.000 100.000% 100.000% 0.000
>= 1 jets w/ Pt>15 987.000 98.700% 99.200% 0.000
Lead Jet Pt>100,|eta|<1.7,EMF<0.9 831.000 83.100% 83.300% 0.000
2nd Lead Jet Pt>100,|eta|<3,EMF<0.9 696.000 69.600% 73.800% 0.000
MHT >= 400 342.000 34.200% 40.800% 53.000
Dphi2 > 0.85 328.000 32.800% 60.600% 0.000
R1 > 0.85 328.000 32.800% 59.500% 0.000
R2 < 3.6 327.000 32.700% 59.300% 0.000
Alpha > 0.5 188.000 18.800% 25.300% 0.000
Dphi1 > 0.9 188.000 18.800% 25.100% 0.000
>= 1 Taus w/ |eta|<2.5 188.000 18.800% 100.000% 0.000
>= 1 Taus w/ Pt>20 188.000 18.800% 98.000% 0.000
>= 1 Taus w/ lead Track 188.000 18.800% 100.000% 0.000
>= 1 Taus w/ lead Track Pt>5 186.000 18.600% 98.600% 1.000
>= 1 Taus passing Track iso. 60.000 6.000% 86.800% 21.000
>= 1 Taus passing ECAL iso. 50.000 5.000% 99.600% 0.000
>= 1 Taus w/ 1||3 Prongs 44.000 4.400% 99.000% 0.000
>= 1 Taus passing e-Veto 34.000 3.400% 100.000% 0.000
>= 1 Taus passing mu-Veto 27.000 2.700% 100.000% 0.000
--------------------------------------------------------------------------------------------------------------------------------------
Example Plots
A root file is also created: plotsSusy.root:
Results for 3X
Table of Efficiencies:
-------------------------------------------------------------------------------------------------------------------------------
Name Events Relative (%) Cumulative (%)
-------------------------------------------------------------------------------------------------------------------------------
TauPt 166749 86.44 +- 0.07795 86.44 +- 0.07795
TauEta 161411 96.8 +- 0.04311 83.67 +- 0.08415
TauSeedTrackPt 148689 92.12 +- 0.06707 77.08 +- 0.0957
TauIso 14986 10.08 +- 0.07807 7.769 +- 0.06094
TauProng 10649 71.06 +- 0.3704 5.52 +- 0.052
TauElecVeto 7300 68.55 +- 0.4499 3.784 +- 0.04344
TauMuonVeto 4371 59.88 +- 0.5737 2.266 +- 0.03388
JetsPt 3767 86.18 +- 0.522 1.953 +- 0.0315
LeadJet 2747 72.92 +- 0.724 1.424 +- 0.02698
SecondLeadJet 1555 56.61 +- 0.9456 0.8061 +- 0.02036
Mht 418 26.88 +- 1.124 0.2167 +- 0.01059
Dphi2 406 97.13 +- 0.8168 0.2105 +- 0.01043
R1 406 100 +- 0 0.2105 +- 0.01043
R2 406 100 +- 0 0.2105 +- 0.01043
Alpha 166 40.89 +- 2.44 0.08605 +- 0.006676
Dphi1 166 100 +- 0 0.08605 +- 0.006676
-------------------------------------------------------------------------------------------------------------------------------
Expected # of Events @ L = 1e+014 ib ---> 0.05186 +- 0.004024
-------------------------------------------------------------------------------------------------------------------------------
Example Plots
OS, LS, & OS-LS plots after Tau ID cuts.
OS, LS, & OS-LS plots after 1st and 2nd Leading Jet Cuts.
OS, LS, & OS-LS plots after Mht Cut.
OS, LS, & OS-LS plots after Dphi2, R1, R2, Alpha, & Dphi1 Cuts.
Results for 4X
Table of Efficiencies
http://roy.physics.tamu.edu/Work/EffTable
Comments on Simplified Model Scans
The generator-level information for the Simplified Model
SUSY (
SMS) scans are in the
LHEEventProduct collection. Code for extracting these parameters has not yet made it into
CVS.
I wrote private code which can study a single point from the Python config (Not yet in
CVS!):
process.analyzeHiMassTau.SinglePoint = cms.bool(True)
process.analyzeHiMassTau.mLSP = cms.double(50.)
process.analyzeHiMassTau.mGL = cms.double(350.)
I then have scripts which can make python config files with differing parameters for the whole scan. These hundreds of config files can then be run simultaneously using Roy's Multicondor.
I then wrote a root macro which forloops over the output root files to make 2D plots of N_events, N_pass, etc (Not yet in
CVS!). I then wrote a root macro which makes nTuples that are compatible with the
HighMassTau fitter from the Z prime analysis (Not yet in
CVS!). I then have a root macro which can loop over points and run the fitter (which only works from the command line for now) with lines such as these:
TString command = "sed 's/blah/"+convertInt(i)+"-"+convertInt(j)+"/' fitter.txt > fitter.cfg";
gSystem->Exec((TString(command)).Data());
TString command = "./runFitter > tmp.txt";
gSystem->Exec((TString(command)).Data());
The final out put of this macro has all of the exclusion plots (Not yet in
CVS!)
Edits and Comments on AN-11-519

--> DONE

--> ONGOING

--> PENDING

--> UNKNOWN
Alfredo (01-12-2012)

l21-24: need to have a stronger statement about the importance of taus. Perhaps we can add that in many models and/or
regions of parameter space, the couplings to third generation sparticles are enhanced and thus taus become important. We can also add a statement about large tanbeta.

l76: change "If an excess ... or the high HT region" --> "If an excess ... in the high HT region"

l78: need a reference to CLs

l109-110: We will be using a scale factor instead of a full data-driven estimation. Therefore, we should say that we measure a scale factor from a QCD enriched sample to correct the MC prediction in the signal region and validate that QCD is indeed a small contribution.

l126: change "4.65" --> "4.6" to be consistent with abstract

l166: change "Particle Flow (PF) objects" --> "Particle Flow (PF) candidates"

l214: change "signal LM benchmark point" --> "signal"

Section 5: Need to update the selections

l265: change "and so that maintain" --> "and to maintain"

l269: change MHT > 200 --> MHT > 250

l271: change MHT > 200 --> MHT > 250

l284: change "benchmark LM2 sample" --> "benchmark sample"

Section 7: we should just take sections 8, 9.1, 9.1.1, and 9.2 of AN-11-164 and put them here.

l250: missing reference and plots (plots and numbers from Roy)

l351: change "purity is close to 100%" --> "purity is high"

l373: missing reference

l375: missing plots

l383: missing reference (appendix of AN-11-164 needs to be added to this AN ... since most of the appendix is based on MC, this will not change much)

l388: missing reference
Teruki (01-14-2012)
Comments on page 1.
I am suggesting the following references (below) and text (jpeg file):

[1]
%%mSUGRA%%
%\cite{msugra}
\bibitem{msugra}A. H. Chamseddine, R. L. Arnowitt, P. Nath, Phys. Rev. Lett. 49, 970 (1982); R. Barbieri,
S. Ferrara, C. A. Savoy, Phys. Lett. B119, 343 (1982); L. J. Hall, J. D. Lykken, S. Weinberg,
Phys. Rev. D27, 2359-2378 (1983); P. Nath, R. L. Arnowitt, A. H. Chamseddine, Nucl. Phys. B227, 121 (1983); For a review, see H. P. Nilles, Phys. Rept. 110, 1-162 (1984);
Stephen P. Martin, "A Supersymmetry Primer" [arXiv.hep-ph/9709356].

[2] R. Arnowitt et al., PRL 100, 231802 (2008) ... this is a paper to study
the signal of stau-neutralino co-annihilation at the LHC

[3] M.Dine and W. Fischler, Phys. Lett. B 110, 227 (1982);
C.R. Nappi and B.A. Ovrut, Phys. Lett. B 113, 175 (1982);
L. Alvarez-Gaum´e, M. Claudson and M.B. Wise, Nucl. Phys. B207, 96 (1982).

[4] E. Komatsu et al.,
ApJS, 192, 18 (2011) .... this is WMAP7 paper

I added Ref 3 for GMSB as another example of model with taus
to address one of Alfredo's suggestion of strengthening physics motivation.
120114_page1.jpg: Teruki's Comment's (01-14-2012)
Comments -----

L192: H/p in italic to be consistent with Table 4

L221&222: MHT > 200 ====> changed to 250

Table 7 and 8: MHT > 200 ===> Chnaged to 250

L264: "OS-LS" .... math mode "-"
Alfredo (01-12-2012)

Section: Need pt and MHT distributions for our benchmark point

Section 7: we should just take sections 8, 9.1, 9.1.1, and 9.2 of AN-11-164 and put them here.

Then we can just update the numbers, tables and plots

Section W+jets background: update description of background estimation method following the ttbar philisophy.
Teruki (01-14-2012)

L241: MHT > 250 in |eta| < 5? ... NO eta cuts

Fig.3 and 4:
JiEun has to provid a good set of plots --> Alfredo will provide

1) Fig. 3 - stay as it is for now. This is based on LM2, but should be similar for new benchmarpoint. ---> New point from Alfredo

2) Figs. 4 and 5 - Alfredo plans to update for new benchmark point.
3) Table 7, 8, 9 - Roy plans to do AFTER he finishes TTBar and others.
4) Table 10 - from Andres

5) Sec. 7.2.2 (Validation in e-tau final state) -- We REMOVED.

6) Tabl 14 (TTbar Extraction) - Roy, please fill the numbers.
7) Sec. 8.2 (Z-->nunu) .. the text is from 1,1 fb-1. Sinjini will have to update Fig. 11, Tables 15 and 16.

8) Sec. 8.3 (QCD) - Will is working on. Will be done by 5-6 pm Tuesday.
9) Table 18 (W+jets) -
JiEun, please double-check and update.
10) Fig. 14(a) .. discrepancy at N(track) = 1, 2, 3, and 4.

11) Figs 15 and 16 - They are plots for testing a bias due to b-tagging. We didn't see a bias. Let's remove two figures from AN. We may have to re-visit again during
ARC review.

additional: updated Fig 1 (Alfredo) and removed Fig 14 (c), 14 (d), line 211
NOTE: we are now using a new benchmark point: m0 = 360, m1/2 = 560, tanB = 40, A0 = -500.
1) Table 7, 8, 9 - Roy plans to do AFTER he finishe his talk..
2) Table 10 & 11 - All numbers are in, except for the systematic errors.
3) L.468 ... missing reference link
4) Sec. 8.2 (Z-->nunu) .. the text is from 1,1 fb-1. Sinjini will have to update Fig. 11, Tables 15 and 16.
5) Table 17 (W+jets) -
JiEun, please double-check the error propagation and update.
L.586 ... missing figure link...
L. 604 .. fix "FIXME"
6) L.610 .. We should have "Systematic Uncertainty" section before "Exclusion Limits" section.
7) We will be ready to be setting limits as soon as #4 and #5 are done.
8) Goal #1: upload AN (w/o limits) on CADI on Jan 19 (Thu)
9) Goal #2: Re-upload AN and PAPER on Jan 26 (Thu).
NOTE: we are now using a new benchmark point: m0 = 360, m1/2 = 560, tanB = 40, A0 = -500.
Tasks
1) Table 7, 8, 9 - Roy plans to do AFTER he finishes his talk..
2) Table 10 & 11 - All numbers are in, except for the systematic errors.
3) L.469 ... missing reference link

4) Table 13 ... we have to remove "1.4_stat". This is placed by mistake, according to Roy.
5) Sec. 8.2 (Z-->nunu) .. the text is from 1,1 fb-1. Sinjini will have to update Fig. 11, Tables 15 and 16.

6) L.555 & L. 560 ... 0.,75 --> 0.74

7) Table 17 (W+jets) and related text -
JiEun, please double-check the error propagation and update.
8) We will be ready to be setting limits as soon as #5 and #7 are done.
9) Goal #1: upload AN (w/o limits) on CADI on Jan 20 (Fri)
10) Goal #2: Re-upload AN and PAPER on Jan 26 (Thu).
NOTE: we are now using a new benchmark point: m0 = 360, m1/2 = 560, tanB = 40, A0 = -500.
Tasks
1) Table 7, 8, 9 - Roy plans to do AFTER he finishes his talk..
2) Table 10 & 11 - All numbers are in, except for the systematic errors.
3) TTbar + Wjets sections:
(*) L. 451 ... have an equation number;
(*) L. 470 ... missing reference link;
. (*) See comment on Eq.10;
(*) L. 496 ... remove "%";
(*) L. 603 ... have an equation number;
L. 611 ... Figure 17.
4) Sec. 8.2 (Z-->nunu) .. the text is from 1,1 fb-1. Sinjini will have to update Fig. 11, Tables 15 and 16.
5) Sec. 10 Systematic studies
6) We will be ready to be setting limits as soon as #4 and #5 is done.
7) Goal #1: upload AN (w/o limits) on CADI on Jan 20 (Fri)
8) Goal #2: Re-upload AN and PAPER on Jan 26 (Thu).

Uploaded AN (w/o limits) on CADI on Jan 21 (Sat) ==> done, Jan 23 (Mon)
NOTE: we are now using a new benchmark point: m0 = 360, m1/2 = 560, tanB = 40, A0 = -500.
Executive Summary
TTbar |
2.0 +/- 0.4 |
(was 2.18 +/- 2.66 (stat+syst) at 1.1 fb-1) |
Wjets |
4.2 +/- 0.6 ("tau fake" method) |
(was 0.00 +/- 1.20 (stat+syst) at 1,1 fb-1) |
QCD |
0.02 +/- 0.02 |
(was 0.58 +/- 0.86 (stat+syst) at 1.1 fb-1) |
Zinv |
in progress, but should be small (Sinjini) |
(was 0.00 +/- 0.16 (stat+syst) at 1.1 fb-1) |
Total |
6.2 |
(was 2.76 at 1.1 fb-1) |
Tasks
1) Table 7, 8, 9 - Roy plans to do AFTER he finishes his talk..
2) Table 10 & 11 - All numbers are in, except for the systematic errors.
3) TTbar + Wjets sections:
(*) L. 451 ... have an equation number (later, due to technical reason);
(*) L. 470 ... missing reference link;
(*) L. 603 ... have an equation number (later, due to technical reason);
4) Sec. 8.2 (Z-->nunu) .. the text is from 1,1 fb-1. Sinjini will have to update Fig. 11, Tables 15 and 16.

5) Sec. 10 Systematic studies (Alfredo)
6) We will be ready to be setting limits as soon as #4 and #5 is done.
7) Goal: Re-upload AN and PAPER on Jan 27 (Fri).
Executive Summary
TTbar |
2.0 +/- 0.4 |
(was 2.18 +/- 2.66 (stat+syst) at 1.1 fb-1) |
Wjets |
4.2 +/- 0.6 ("tau fake" method) |
(was 0.00 +/- 1.20 (stat+syst) at 1,1 fb-1) |
QCD |
0.02 +/- 0.02 |
(was 0.58 +/- 0.86 (stat+syst) at 1.1 fb-1) |
Znunu |
0.03 +/- 0.02 |
(was 0.00 +/- 0.16 (stat+syst) at 1.1 fb-1) |
Ztautau |
0.64 +/- 0.43 |
n.a. |
Total |
6.89 |
(was 2.76 at 1.1 fb-1) |
XX observed.
Tasks
1) Table 7, 8, 9 (Roy/Will) -
http://cern.ch/go/Wf86
2) Table 10 & 11 - All numbers are in, except for the systematic errors.
3) TTbar + Wjets sections:
(*) L. 451 ... have an equation number (later, due to technical reason);
(*) L. 470 ... missing reference link;
(*) L. 603 ... have an equation number (later, due to technical reason);
4) Sec. 8.2 (Z-->nunu) .. DONE, but the text, Fig. 11, Tables 15 and 16 are from 1,1 fb-1.
5) mSUGRA and SMS_T1tauh patTuples/log files
(*) /afs/cern.ch/user/g/gurrola/public/SMST1tauh.log
(*) /afs/cern.ch/user/g/gurrola/public/mSUGRA.log
7) Goal: Re-upload AN and PAPER on Jan 27 (Fri).
%ENDTW
Tasks
1) Table 7, 8, 9 (Roy/Will) -
http://cern.ch/go/Wf86
2) *
120124_Will_SusyTau_p2.pdf: QCD estimate (David Stuart's comment)
3) mSUGRA and SMS_T1tauh patTuples/log files
(*) /afs/cern.ch/user/g/gurrola/public/SMST1tauh.log
(*) /afs/cern.ch/user/g/gurrola/public/mSUGRA.log
4) Goal 1: Re-upload AN on Jan 25 (Wed) for David's and Eva's review
5) Goal 2: Re-upload AN on Jan 27 (Fri) for
ARC's review
6) Goal 3: Re-upload AN and PAS on Jan 31 (Tue) for Pre-Approval
Edits and Comments on AN-11-485
--
AlfredoGurrola - 29 Jul 2009