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6. Other Detector Technologies
JLC/NLC/TESLA have different detector options due to accelerator-parameter differences and different strategies.
Grand-design Options
Major Detector Options
- VTX
- CCD (JLC/NLC/TESLA) ; smallest pixel size , thinnest , slow readout , sensitive to radiation damage
. . . . . . Slowness may not be good for TESLA
- CMOS Active Pixel ; small pixel size, thin, fast readout, radiation-hard, small chip-size
- Hybrid Active Pixel ; modest pixel size, thick, fast readout, radiation-hard
- IT
- Si-strip (JLC/NLC/TESLA)
- SciFi . . . for better timing resolution.
- CT
- Jet (JLC) . . . (Long) Wires are always troublesome ; Not a 3-D measurement.
- TPC (NLC-L/TESLA) . . . Huge readout channel,
Timing resolution for bunch-ID may be challenging for NLC.
- Si-drift/Si-strip (NLC-SD) . . . less hit-redundancy, kink-track may be troublesome.
- CAL
- Tile/fiber (JLC/NLC-L/TESLA-HCAL). . . fine granularity, modest cost, well-establised technique
- W/Si + Digital (TESLA/NLC-SD) . . . ultimate granularity, very expensive (W/Si), developing technique
- Crystal EM . . . coarse longitudinal granularity, excellent energy resolution, expensive, well-established technique.
Other sub-detectors do not have arguing options.
Need to clarify what we must achieve at least and what we can do best,
with boundary conditions of budget, effort, time-span.
Full-simulation study heavily needed, and not enough at all so far.
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yoshiaki.fujii@kek.jp, July 10,2002 at 5th ACFA LCWS at Tokyo