1 |
sunanda |
1.1 |
\section{Triggers to be Used}
|
2 |
|
|
|
3 |
sunanda |
1.2 |
Isolated charged particles can be obtained from minimum bias events.
|
4 |
|
|
However with the increase in the luminosity of the machine, the minimum
|
5 |
|
|
bias events will be highly suppressed by some large prescale factors in
|
6 |
|
|
the trigger. So minimum bias trigger can be considered only at low
|
7 |
|
|
luminosities. There are two basic requirements in these measurements:
|
8 |
|
|
\begin{enumerate}
|
9 |
|
|
\item Measurement of response of low momentum particles need to be made
|
10 |
|
|
with the hadron calorimeter read out with no zero suppression
|
11 |
|
|
scheme. This is needed to overcome the strong nonlinear behaviour
|
12 |
|
|
of calorimeter response at lower energies.
|
13 |
|
|
\item Calibration of the hadron calorimeter requires large number of
|
14 |
|
|
tracks with sufficiently high energy and non-interacting in the
|
15 |
|
|
electromagnetic calorimeter.
|
16 |
|
|
\end{enumerate}
|
17 |
|
|
|
18 |
|
|
Rate for low energy particles is fairly large; but a dedicate trigger may
|
19 |
|
|
be needed to have HCAL readout in a special mode. Rate for high momentum
|
20 |
|
|
tracks is smaller and prescale for the jet triggers will significantly
|
21 |
|
|
cut this rate further. So a dedicated high level trigger may be useful
|
22 |
|
|
to provide a comfortable rate for isolated high momentum hadrons.
|