TauPlusJets2012
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Twiki:
-Top
Working Group
-TopCrossSectionTauJetsChannel
-TopCommonScales
-TopCommonObjects
-TopSystematicUncertainties
-TopRootCoreRelease
-TopD3PDProductions
- D3PDContent
-TopInputsD3PDMaker
- TopTauObjects
-
TauRecommendationsWinterConf2013
-
DataPreparationCheckListForPhysicsAnalysis
-GRL
Twiki
-GRL
SVN
- Tau
Working Group
-Susy2012
-
HSG6Analysis2012
SVN Repository:
- Ahmed
Hasib
- Catrin
Bernius
Monte Carlo & Data Samples:
- MC
signal and background samples for analysis.
- TopMC2012
(Signal samples:
ttbar Baseline and Systematic Samples)
-
TopData2012
: For recommendations look at
Top
Reconstruction Group and
Top
GRL
-
ATLAS
Monte Carlo Working Group
- The x-section and filt. efficiency (FE) values from AMI
should be used for reference. In the sample lists the product
of the FE*x-section is passed. The exception are the cases
when sample x-section is not filled to AMI correctly and has
not been manually corrected. In this case a note is passed in
the sample lists below. See here for AMI command line querry tips.
- The following content is automatically filled in the twiki
tables:
- Brief : brief string describing the
sample (automatically extracted)
- Channel : decay channel:
(automatically extracted)
- ttbar options:
- AllHadronic: both t and tbar decay to hadrons
- DiLepton : both t and tbar decay to leptons,
lepton = e,mu,tau
- NoAllHadronic : at least one of t and tbar
doesn't decay to hadrons (directly)
- MC Generator : generator string
(automatically extracted). "Pythia" or "fPythia" refer to
Pythia6 unless "Pythia8" is explicitly stated. Similar for
"Herwig" or "fHerwig" vs "HerwigPP" or "Herwig++".
- DSID : dataset ID. Click on it to
view the sample jO file.
- Nominal Size : the requested number
of reconstructed events (= size of AOD). If the entry is 0
the AOD exists but no events are available. If the entry
is blank then the AOD does not exist. (automatically
extracted)
- FE x-sec [pb]* : filtering efficiency
(branching ratio) times the cross-section (automatically
obtained from AMI unless specified otherwise)
- K-factor : K-factor obtained from the
reference x-section and the FE* x-sec [pb] field
(automatically extracted)
- Reference x-sec: link to reference
x-section article or twiki (set as table input)
- Production link: link to the
sample-related tasks data in the production system
database (automatically extracted)
- AMI EVGEN: link to evgen (most
informative for MC aspects...)-level AMI info
(automatically extracted)
- AMI AOD: link to AOD (automatically
extracted)
- AMI NTUP_TOP: link to the Top D3PD
(automatically extracted)
- Comm: comment field (set as table
input)
Sample Notes
Generator used for the largest fraction of the samples is
MC@NLO+Herwig/Jimmy. Note that MC@NLO
samples have event weight. Each event has a weight of +1 or
-1. Only the sum of the weights is a physical quantity. If
you are calculating the integrated luminosity for the
sample, your numerator should be the sum of the weight.
While the default generator to be used for the analysis is
MC@NLO+Herwig/Jimmy the ttbar samples are also generated
with a variety of other MC generators.
• Pythia and Herwig:
Both of these general purpose generators contain
a large number of built-in processes which are generated
at the lowest QCD order, therefore they are at
fixed leading-order. However, they provide reduced
accuracy in multi-parton final states as they handle QCD
and QED radiations only at the parton shower evolution
(see next paragraphs). Therefore, they are not the primary
choice for the generation of events. In the analysis
presented here Herwig is used only for the generation of
di-boson events.
• AlpGen:
The AlpGen generator is a leading-order matrix
element generator specialized for multi-parton final
states (2 → N). In contrast to Pythia and Herwig, it
provides a more accurate description by using perturbation
theory on all the relevant tree-level Feynman diagrams
with a fixed number of outgoing partons. The result is
bare partons and therefore an additional simulation
package must be interfaced to handle subsequent processes.
This generator is used to simulate the backgroundW+jets,
Z+jets and QCD multi-jet processes up to five outgoing
partons.
• Sherpa:
Similar to AlpGen it provides a more accurate description
of multi-parton final states based on matrix element
calculation. However, it can also handle internally
the rest of the processes without needing to couple with
an external package. In this thesis, W+jets events
generated with this generator are used for systematic
studies.
• AcerMC:
Also a leading-order generator, the AcerMC provides a
library of matrix-element calculation of a number of
built-in processes. Primarily aimed for background
processes
with a large number of partons in the final state, such as
W+jets and Z+jets, it can also be used for the simulation
of t¯t events. Simulated ttbar events using AcerMC are
used for the systematic studies of ISR/FSR effects
• MC@NLO
and POWHEG: The only generators in this
thesis that provide both real and virtual corrections in
the generation process at next-to-leading order. Primarily
used
for the production of top quark events. The MCatNLO is
used to generate the signal events for the ttbar
cross-section analysis, while POWHEG is used for
systematic studies.
MC@NLO is also used for generation of the single-top
events.
Presentation Slides:
- Analysis
Code, SVN and Trigger: July 13, 2012
- Status
of TauPlusJets2012 Code: July 27, 2012
- Status
of TauPlusJets2012 Code: Aug 03, 2012
Papers:
Measurement of the
ttbar production cross section in the final state
with a hadronically decaying tau lepton and jets
using the ATLAS
detector: ATLAS-CONF-2012-032 March 12, 2012
Measurement of the ttbar production
cross section in the tau + jets channel using the ATLAS
detector
Important Indico Pages:
Object Selection
Notes
- For TOP2012 we may keep 2011 isolation cuts, while a full
re-optimization of the 2012 isolation cuts (also considering
mini-isolation as candidate) is being pursued
RootCorePackages2012
egammaAnalysisUtils-00-03-61 I'm using the
tag version 00-03-79 currently.