Changeset 515 in svn for trunk/paper/notes.tex
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- Jul 23, 2009, 11:01:14 PM (15 years ago)
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trunk/paper/notes.tex
r508 r515 671 671 \subsection{\texorpdfstring{$\tau$}{\texttau}-jet efficiency} 672 672 Due to the complexity of their reconstruction algorithm, $\tau$-jets have also to be checked. 673 Table~\ref{tab:taurecoefficiency} lists the reconstruction efficiencies for the hadronic $\tau$-jets in the \textsc{cms} experiment and in \textsc{Delphes}. Agreement is good enough to validate also this reconstruction. 673 Table~\ref{tab:taurecoefficiency} lists the reconstruction efficiencies in \textsc{Delphes} for the hadronic $\tau-$jets from $H,Z \rightarrow \tau^+ \tau^-$. The mass of the Higgs boson is set successively to $140$ and $300~\textrm{GeV}/c^2$. The inclusive gauge boson productions ($pp \rightarrow HX$ an 674 d $pp \rightarrow ZX$) are performed with \textsc{MadGraph/MadEvent} and the $\tau$ lepton decay and further hadronisation are handled by \textsc{Pythia/ 675 Tauola}. All reconstructed $\tau$-jets are $1-$prong, and follow the definition described in section~\ref{btagging}, which is very close to an algorithm 676 of the \textsc{cms} experiment~\cite{bib:cmstauresolution}. At last, corresponding efficiencies published by the \textsc{cms} and \textsc{atlas} experim 677 ents are quoted for comparison. The agreement is good enough at this level to validate the $\tau-$reconstruction. 678 679 680 681 674 682 675 683 \begin{table}[!h] 676 684 \begin{center} 677 \caption{Reconstruction efficiencies of $\tau$-jets in decays from $Z$ or $H$ bosons, in \textsc{Delphes} and in the \textsc{cms} experiment~\cite{bib:cmstauresolution}.\vspace{0.5cm}} 678 \begin{tabular}{lll} 685 \caption{Reconstruction efficiencies of $\tau$-jets in $\tau^+ \tau^-$ decays from $Z$ or $H$ bosons, in \textsc{Delphes}, \textsc{cms} and \textsc{atlas 686 } experiments~\cite{bib:cmstauresolution,bib:ATLASresolution}. Two scenarios for the mass of the Higgs boson are investigated. Events generated with \textsc{MadGraph/MadEvent} and hadronised with \textsc{Pythia}. The decays of $\tau$ leptons is handled by the \textsc{Tauola} version embedded in \textsc{Pythia}.\vspace{0.5cm}} 687 688 \begin{tabular}{lrl} 679 689 \hline 680 \multicolumn{2}{c}{\textsc{cms}} & \\ 681 $Z \rightarrow \tau^+ \tau^-$ & $38 \%$ & \\ 682 $H \rightarrow \tau^+ \tau^-$ & $36 \%$ & $m_H = 150~\textrm{GeV}/c^2$ \\ 683 $H \rightarrow \tau^+ \tau^-$ & $47 \%$ & $m_H = 300~\textrm{GeV}/c^2$ \\ 684 \multicolumn{2}{c}{\textsc{Delphes}} & \\ 685 $H \rightarrow \tau^+ \tau^-$ &$42 \%$ & $m_H = 140~\textrm{GeV}/c^2$ \\ 690 & \textsc{cms}&\textsc{Delphes} \\ 691 $Z \rightarrow \tau^+ \tau^-$ & $38.2\%$ & $32.4\pm1.8\%$ \\ 692 $H(140) \rightarrow \tau^+ \tau^-$ & $36.3\%$ & $39.9\pm1.6\%$ \\ 693 $H(300) \rightarrow \tau^+ \tau^-$ & $47.3\%$ & $49.7\pm1.5\%$ \\ 694 & \textsc{atlas}&\textsc{Delphes} \\ 695 $Z \rightarrow \tau^+ \tau^-$ & $33\%$ & $28.6\pm 1.9\%$ \\ 696 $H(140) \rightarrow \tau^+ \tau^-$ & & $32.8\pm 1.8\%$ \\ 697 $H(300) \rightarrow \tau^+ \tau^-$ & & $43.8\pm 1.6\%$ \\ 698 686 699 \hline 687 700 \end{tabular}
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