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root/cvsroot/UserCode/sunanda/CaloTaskRep10/triggers.tex
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# Content
1 \section{Triggers to be Used}
2
3 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.