Diff for /ttbar/p20_taujets_note/Abstract.tex between versions 1.1.1.1 and 1.2

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 This note presents a new measurement of $p\bar p \to t \bar tX$ production   We present a new measurement of $p\bar p \to t \bar tX$ production 
 at $\sqrt{s}=1.96$ TeV using 4951.86 pb$^{-1}$ of data collected with the  at $\sqrt{s}=1.96$ TeV using 4951.86 pb$^{-1}$ of data collected with the
 D\O\ detector between 2002 and 2010. We focus on the final state  D0 detector between 2002 and 2010. We focus on the final state
 where the $W$ boson from one of the top quarks decays into a   where the $W$ boson from one of the top quarks decays into a 
 $\tau$ lepton and its associated neutrino, while the other W boson decays into   $\tau$ lepton and its associated neutrino, while the other $W$ boson decays into 
 a quark-antiquark pair. We aim to select those events in which the  a quark-antiquark pair. We aim to select those events in which the
 $\tau$ lepton subsequently decays hadronically, meaning to one or three charged hadrons, zero  $\tau$ lepton subsequently decays hadronically, meaning to one or more charged hadrons, zero
 or more neutral hadrons and a tau neutrino. We use a neural network b-tagging algorithm  or more neutral hadrons and a tau neutrino. We train a topological neural network 
 as well as a topological neural network to enhance signal over the background. For a top quark  as the method to enhance signal over the background. For a top quark
 mass of 172.5 GeV the preliminary result for the measured cross section is:  mass of 172.5 GeV we measure the cross section to be:
   
 \begin{center}\[\sigma (t\overline{t}) =   \begin{center}\[\sigma (t\overline{t}) = 
 8.46\;\;_{-1.04}^{+1.06}\;\;({\textrm{stat}})\;\;_{-0.88}^{+0.92}\;\;({\textrm{syst}})\;\;\pm 0.3\;\;({\textrm{lumi}})\;\; \rm{pb.}\]  8.46\;\;_{-1.04}^{+1.06}\;\;({\textrm{stat}})\;\;_{-0.78}^{+0.84}\;\;({\textrm{syst}})\;\;\pm 0.3\;\;({\textrm{lumi}})\;\; \rm{pb.}\]
 \par\end{center}  \par\end{center}
   

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