1 |
friis |
1.7 |
The tau identification strategy described previously can be extended by
|
2 |
|
|
looking at the different hadronic decay modes of the tau individually.
|
3 |
|
|
The dominant hadronic decays of taus consist of a one or three charged
|
4 |
|
|
$\pi^{\pm}$ mesons and up to two $\pi^0$ mesons and are enumerated in
|
5 |
friis |
1.6 |
table~\ref{tab:decay_modes}. The majority of these decays proceed through
|
6 |
friis |
1.3 |
intermediate resonances and each of these decay modes maps directly to a tau
|
7 |
|
|
final state multiplicity. Each intermediate resonance has a different invariant
|
8 |
friis |
1.5 |
mass (see figure~\ref{fig:trueInvMass}). This implies that the problem of
|
9 |
friis |
1.7 |
hadronic tau identification can be re-framed from a global search for
|
10 |
|
|
collimated hadrons satisfying the tau mass constraint into a ensemble of
|
11 |
|
|
searches for single production of the different hadronic tau decay resonances.
|
12 |
|
|
The Tau Neural Classifier algorithm implements this approach using two
|
13 |
|
|
complimentary techniques: a method to reconstruct the decay mode and an
|
14 |
|
|
ensemble of neural network classifiers used to discriminant the individual
|
15 |
|
|
decay modes.
|
16 |
friis |
1.1 |
|
17 |
|
|
\begin{table}
|
18 |
|
|
\centering
|
19 |
|
|
\begin{tabular}{ l c r r }
|
20 |
friis |
1.3 |
Visible Decay Products & Resonance & Mass (M$e$V/$c^2$) &
|
21 |
friis |
1.5 |
Fraction~\cite{pdg} \\
|
22 |
friis |
1.1 |
\hline
|
23 |
friis |
1.7 |
$\pi^{-}$ & - & 135 & 10.9\% \\
|
24 |
friis |
1.3 |
$\pi^{-}\pi^0$ & $\rho$ & 770 & 25.5\% \\
|
25 |
|
|
$\pi^{-}\pi^0\pi^0$ & $a1$ & 1200 & 9.3\% \\
|
26 |
|
|
$\pi^{-}\pi^{-}\pi^{+}$ & $a1$ & 1200 & 9.03\% \\
|
27 |
|
|
$\pi^{-}\pi^{-}\pi^{+}\pi^0$ & $a1$ & 1200 & 4.5\% \\
|
28 |
friis |
1.1 |
\hline
|
29 |
friis |
1.3 |
Total & & & 59.2\% \\
|
30 |
|
|
\hline
|
31 |
|
|
Other hadronic modes & & & 5.59\% \\
|
32 |
friis |
1.1 |
\end{tabular}
|
33 |
friis |
1.3 |
\label{tab:decay_modes}
|
34 |
|
|
\caption{Resonances and branching ratios of the dominant hadronic decays of
|
35 |
friis |
1.7 |
the tau lepton. The decay products listed correspond to a negatively
|
36 |
|
|
charged tau lepton; the table is identical under charge conjugation.}
|
37 |
friis |
1.1 |
\end{table}
|
38 |
|
|
|
39 |
friis |
1.3 |
\begin{figure}[t]
|
40 |
|
|
\begin{center}
|
41 |
friis |
1.4 |
\includegraphics[width=90mm]{figures/truthIMvsDM.pdf}
|
42 |
friis |
1.3 |
\end{center}
|
43 |
|
|
\caption{The invariant mass of the visible decay products in hadronic tau
|
44 |
|
|
decays. The decay mode $\tau^{-} \rightarrow \pi^{-} \nu_\tau$ is omitted.
|
45 |
|
|
The different decay modes have different invariant masses corresponding to
|
46 |
|
|
the intermediate resonance in the decay.}
|
47 |
|
|
\label{fig:trueInvMass}
|
48 |
|
|
\end{figure}
|