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Additional resources for Calorimetry in Particle Physics: Proceedings of the Tenth International Conference, California, USA 25-29 March 2002
Status of CMS HF Quartz Fiber Calorimetry. Y. Onel. Presentation to this conference. 21.
3% rms cell to cell dispersion) can be obtained with data recorded during 48 hours at low luminosity (where the rate of 2 -+ e+e- is about 1 Hz). The same constraint gives indeed an extremely precise absolute energy scale calibration. In CMS the crystals are first calibrated in the laboratory with laser pulses 28 and/or radioactive sources. Experience shows that the correlation of this calibration with the response to high energy electrons from beam tests is not better than 6% rms. In the likely c a e that all crystals cannot be calibrated in test beam, the in-situ inter-calibration will use lab results as starting point.
4. 1. A harsh region The first ”raison d’i5tre” of forward calorimetry is to avoid tails due to particles escaping around the beam pipe, in the measurement of missing ET. For practical reasons, it is difficult to instrument beyond q =5. This is in general adequate, although some channels where precise measurement of ET is necessary would benefit from an extended coverage (H+ TT at low luminosity is such an example). At shower max and q = 4, in ATLAS, the neutron flux is about 3 1015n/cm2/year, a factor 1000 above the barrel EM situation.