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[Rivet-svn] rivet: 4 new changesetsRivet Mercurial rivet at projects.hepforge.orgTue Feb 23 22:00:01 GMT 2016
details: https://rivet.hepforge.org/hg/rivet/rev/5ecfafbeea95 branches: release-2-4-x changeset: 4991:5ecfafbeea95 user: Andy Buckley <andy at insectnation.org> date: Tue Feb 23 21:04:17 2016 +0000 description: Adding CMS pseudotop analysis details: https://rivet.hepforge.org/hg/rivet/rev/cb9b822cdfa9 branches: release-2-4-x changeset: 4992:cb9b822cdfa9 user: Andy Buckley <andy at insectnation.org> date: Tue Feb 23 21:48:50 2016 +0000 description: Merge PseudoJet code locally into CMS analysis, and revert C++11 features for now -- compiles details: https://rivet.hepforge.org/hg/rivet/rev/f8c1b2db0097 branches: release-2-4-x changeset: 4993:f8c1b2db0097 user: Andy Buckley <andy at insectnation.org> date: Tue Feb 23 21:50:42 2016 +0000 description: DOS -> Unix newline normalisation details: https://rivet.hepforge.org/hg/rivet/rev/70169c1556bd branches: release-2-4-x changeset: 4994:70169c1556bd user: Andy Buckley <andy at insectnation.org> date: Tue Feb 23 21:54:30 2016 +0000 description: Hide analysis prep directory diffs (truncated from 1610 to 50 lines): --- a/.hgignore Tue Feb 23 17:08:18 2016 +0000 +++ b/.hgignore Tue Feb 23 21:54:30 2016 +0000 @@ -67,3 +67,4 @@ ^a\.out\.dSYM$ ^Rivet-.\..\..$ ^local/.*$ +^analyses\d\d\d$ --- /dev/null Thu Jan 01 00:00:00 1970 +0000 +++ b/data/anainfo/CMS_2015_I1370682.info Tue Feb 23 21:54:30 2016 +0000 @@ -0,0 +1,71 @@ +Name: CMS_2015_I1370682 +Year: 2015 +Summary: Comparisons of Theory Predictions for the ttbar Process with Data from pp Collisions at $\sqrt{s}$ = 8 TeV +Experiment: CMS +Collider: LHC +InspireID: 1370682 +Status: VALIDATED +Authors: + - Javier Fernandez <Javier.Fernandez at cern.ch> + - Jungwan John Goh <Junghwan.Goh at cern.ch> + - Efe Yazgan <efe.yazgan at cern.ch> + - Markus Seidel <markus.seidel at cern.ch> + - James Keaveney <james.keaveney at vub.ac.be> + - Elvire Bouvier <e.bouvier at cern.ch> + - Benedikt Maier <benedikt.maier at cern.ch> +References: + - Eur.Phys.J. C75 (2015) 542: For the analysis + - CMS-PAS-TOP-15-011 : For details about the Rivet implementation +RunInfo: + pp QCD interactions at $\sqrt{s} = 8$ TeV. Data collected by CMS during the year 2012. +Luminosity: 19.7 /fb +Beams: [p+, p+] +Energies: [8000] +Description: + 'The reconstruction of particle-level top quarks and anti-quarks is implemented in this module. Measurements at $sqrt{s} = 8 TeV are based on parton-level information in the full phase space using MADGRAPH+PYTHIA6. To match the particle-level top quark distributions to the measurements unfolded to the parton-level, a correction function to the particle-level distributions, derived using the same MADGRAPH+PYTHIA6 configuration that was used for the original measurement of the data points, ias applied. Using the same MC configuration as used for the unfolding to correct back the parton-level to particle-level, the model dependence introduced in unfolding to parton-level and extrapolating the measurement to the full phase space is eliminated. + +In this analysis, the particle-level top quark is defined using the following particle definitions: +\begin{itemize} +\item{Dressed lepton} : An object constructed by applying the anti-$k_{T}$ jet clustering~\cite{antikt} with a distance parameter of $R=0.1$ to the collection of final state electrons, muons and photons that do not originate from hadron decays. +The clustered objects that pass the acceptance cuts (\pt $> 20$ GeV and $|\eta| < 2.4$) are considered. +\item{Prompt neutrino} : A neutrino that does not originate from a hadronic decay. +\item{Ghost B hadron} : A weakly decaying hadron with B flavor and its decay products are selected. +Since both the B hadron and its decay products are included, the momenta of the B hadron is rescaled by a very small factor ($10^{-20}$) to be used in the jet clustering. This avoids double-counting, but retains information about the origin of the decay products. +\item{Jet} : A jet is constructed applying the anti-$k_{T}$ jet clustering algorithm with a distance parameter of $R=0.5$ to the collection of all particles except neutrinos and constituents of dressed leptons. For the generator level b-jet finding, ghost B hadrons are also added to the jet clustering. Jets are required to pass acceptance cuts of \pt$ > 30$ GeV and $|\eta| < 2.4$. +\item{b-jets} : b-quark jets are defined as the jets with a Ghost B hadron among their constituents. +\end{itemize} + +Based on the particle-level objects defined above, W bosons and top quarks are reconstructed using W boson and top quark mass constraints, respectively, as described below: +\begin{itemize} +\item{particle-level W boson pair} : Combinations of dressed lepton and prompt neutrinos are made to reconstruct the particle-level $W$ boson candidate that decays to a lepton-neutrino pair. The same is done with jets without B hadrons to reconstruct the $W$ boson decaying hadronically.
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