TauPlusJets2012  

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ATLAS Physics

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- D3PDContent
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- TauRecommendationsWinterConf2013
 
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-GRL Twiki
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Tau Working Group
 
-Susy2012

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HSG6Analysis2012

-TopETmissFall2012

- METUtilityAthena


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

 
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

RootCorePackages2012

egammaAnalysisUtils-00-03-61 I'm using the tag version 00-03-79 currently.