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1   %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
2   \section{Introduction}\label{section:Intro}
3   %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
4 < This note describes an independent search for $H \rightarrow ZZ$ decays in the 4-lepton channel.  Currently the analysis is performed in the context of the $1.6~\rm{fb^{-1}}$ LP dataset.  We consider two kinematic scenarios, consistent with the direction of the baseline $4\ell$ analysis~\cite{ref:baseline}.  The primary differences in this analysis with respect to the current baseline are :
4 > This note describes a search for $H \rightarrow ZZ^{*}$ in the 4-lepton channel with $4.7~\rm{fb^{-1}}$.  The primary differences between this analysis and the current baseline~\cite{baseline} are :
5  
6   \begin{itemize}
7 \item {\bf MVA Electron Identification :} Electrons are identified using a Boosted Decision Tree discriminant trained on samples of candidates from data.
7  
8 < \item {\bf Variable Electron Identification Working Points :} Electron candidates that form the on-shell Z in the 4 lepton system are selected with a looser set of ID requirements relative to those forming the off-shell Z.
8 > \item {\bf MVA Electron Identification :} Electrons are identified using a Boosted Decision Tree discriminant trained on data.  Identification requirements are looser for electron canidates used in the reconstruction of the on-shell $Z$.
9  
10 < \item {\bf Anuglar Discrimination :} We include angular information in the signal extraction fit via an MVA discrminant.
12 <
13 < \end{itemize}
10 > \item {\bf 2D Signal Extraction :} We include angular information and the mass of the second (potentially off-shell) $Z$ in the signal extraction fit via an MVA discriminant.
11  
12 + \item {\bf Isolation :}  We apply PF isolation criteria on individual leptons.
13  
14 < Pay particular attention to jet backgrounds, which are difficult to estimate and can be sneaky.
14 > \item {\bf Treatment of Fake/Instrumental Backgrounds :} We produce a combined estimate of light and heavy flavor backgrounds using the ``fakeable object'' technique.  We assess the performance of this method in several control regions.
15  
16 < Our analyses differ on several addtional points ({\it e.g.: } application of lepton isolation, fake and heavy flavor background estimation, {\it etc} ), which we explain in the text that follows.  Some aspects of the analysis are not yet complete.  The text describes our strategy for these missing pieces.
16 > \end{itemize}
17  
18 < Overall, our changes to event seleation result in {\bf +9/-4 } events in the loose-kinematics signal region.  We discusse these events in detail in Section~\ref{section:Results}.  The limits we extract are comparable to those of~\cite{ref:baseline} for Higgs masses below $\sim 200~\rm{GeV}$, but improve for higher masses ({\bf Verify}).
18 > These changes result in the selection of {\bf $+13/-20 = 7$ } events with respect to the baseline analysis.  We discuss these events in detail in Section~\ref{sec:Results}.  Our observed limits are comparable to those of~\cite{baseline}.
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