A diagram of the OPAL detector is shown in figure 2.2. Indicated on the diagram is the OPAL co-ordinate system. The electrons and positrons travel along the beam pipe and are bought into collision within the detector. The z-axis is parallel to the beam pipe and positive in the direction of the electrons' momentum. The x-axis indicated in figure 2.2 is taken as positive in the direction pointing towards the centre of the LEP ring.
The main features of the OPAL detector are shown in figure 2.2, and they can concisely be described as follows:
A central detector, consisting of vertex and tracking subdetectors
and surrounded by a solenoid. The central detector provides measurements of the
particle's direction and momentum and their identification by dE
dx as well
as
reconstruction of primary and secondary vertices at and near the interaction
region. The solenoid causes bending of the charged particles in the
tracking chamber.
An electromagnetic calorimeter to provide identification of photons
and electrons and to measure their energy.
A hadronic calorimeter to measure hadronic energy. This is
implemented by measuring the total absorption using instrumentation which
incorporates the magnetic yoke.
A Muon detector to identify muons by measurement of their position
and direction within and behind the hadron calorimeter.
A forward detector, situated in the very forward direction, and used
to measure the received LEP luminosity at OPAL using Bhabha scattering events.
A representation of the cross-section of the OPAL detector can be seen in figure 2.3. A detailed description of each OPAL subdetector is beyond the bounds of this thesis, however, a brief overview of each subdetector is given for completeness. A complete and detailed description of the OPAL detector and all its constituent parts can be found in [14].