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\citation{Charged Higgs Theory}
\citation{CDF Charged Higgs}
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\@writefile{lot}{\contentsline {table}{\numberline {I}{\ignorespaces Background sources, relevant for the $\tau +jets$ analysis. The branching fraction into hadronic $\tau $ has been applied}}{4}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces $\not \tmspace  -\thinmuskip {.1667em}\tmspace  -\thinmuskip {.1667em} E_{T}$ significance for QCD-dominated data (black), $W+jets$ (blue) and $t\mathaccentV {bar}016{t}\rightarrow \tau +jets$ (red).}}{5}{}}
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\@writefile{lot}{\contentsline {table}{\numberline {II}{\ignorespaces Preselection results. Shown are the total acceptances (including preselection) and the number of events scaled to 349 $\pm $ 23 pb$^{-1}$ (no systematic uncertainties except for this luminosity error are included). The ALPGEN samples generation cuts are described in \cite  {l+jets}. An estimate of QCD background not included.}}{5}{}}
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\@writefile{lot}{\contentsline {table}{\numberline {V}{\ignorespaces $b$-tagging and $\tau $ ID results per type after the $\eta $ cut (as explained in section V\tmspace  +\thinmuskip {.1667em}C{}{}{}\hbox {}). Shown are the number of events predicted in signal and observed in the data. An estimate of QCD background is not included.}}{6}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Fit of the $\eta $ and $p_{T}$ distributions of the $\tau $ fake rate.}}{7}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces The 2D combined fit (in $\eta $ and $p_{T}$) of the $\tau $ fake rate.}}{7}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces Result of applying the NN cut. $t\mathaccentV {bar}016{t}$, $W$ and QCD are plotted incrementally in order to compare with the number of events observed in data. Error bars include only statistical uncertainties. $\sigma (t\mathaccentV {bar}016{t})=5.54$ pb is assumed. The right plot only shows the entries at high values of NN cut. }}{8}{}}
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\@writefile{lot}{\contentsline {table}{\numberline {VII}{\ignorespaces Systematic uncertainties on $\sigma (t\mathaccentV {bar}016{t})$ (in pb).}}{9}{}}
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\bibcite{CDF Charged Higgs}{{2}{}{{}}{{}}}
\bibcite{D0 Charged Higgs}{{3}{}{{}}{{}}}
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\bibcite{alljet}{{5}{}{{}}{{}}}
\bibcite{d0det}{{6}{}{{}}{{}}}
\bibcite{PDG}{{7}{}{{}}{{}}}
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\bibcite{l+jets}{{16}{}{{}}{{}}}
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\@writefile{toc}{\appendix }
\@writefile{toc}{\contentsline {section}{\numberline {A}Kinematic Distributions}{10}{}}
\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces 2 of the 5 input variables of the first topological NN before the NN cut ($\tau $ type 2). The Kolmogorov-Smirnov (KS) probabilities are shown, indicating the quality of the agreement.}}{10}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {7}{\ignorespaces The resulting output of the second (final) NN ($\tau $ type 2).}}{10}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {8}{\ignorespaces The resulting output of the second (final) NN ($\tau $ type 3).}}{11}{}}
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