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The electron hodoscope will be instrumented as a detector system which can
operate independently or in coincidence with the chamber system. The array consists
of inner and outer scintillators. Each detector slab is about 84 cm long and
14 cm wide. Each element will be read out on both sides with photomultiplier
tubes. This allows reconstruction of the
(detector element) and
z position (time difference) of the electron trajectory. We plan both analog
(using MHz wave form digitizer) as well as digital readout (using CAEN TDC's) of
the detectors. The scintillator is a simplified version of the proposed MuLan
detector. We hope to exploit the synergy between the two projects both in detector
hardware and the above mentioned analog readout.
Within the next few months the following studies to define the final geometry
of the hodoscope elements will take place.
- We will test prototypes of different thickness (3 mm to 1 cm) to study the light
collection efficiency and homogeneity. Good collection efficiency allows low
discriminator thresholds, which reduce our sensitivity to threshold/stability
variations. Although this sensitivity is less critical in a dc experiment than
in a pulsed mode, it still should be kept as small as possible.
- The end face of the scintillator has a very similar size as the MuLan tiles.
Thus we will use similar lightguides and phototubes. In order to finalize the
light guide design we plan to compare to the collection properties of the light
coupling using a 45
reflective mirror to ideal adiabatic strips.
The 64 phototubes of the electron hodoscope will each have their own CAEN TDC channel.
Sufficient discriminator channels are available at UIUC. The z resolution will
be limited by the relatively poor TDC bin width of 1.6 ns. The analog readout
will allow a time resolution of
0.2 ns. Moreover it also permits walk and attenuation
corrections as well as careful pile-up studies.
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Peter Kammel
2001-02-04