By Ren-Yuan Zhu
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H. Brueckmann et al, NIM A263, 136 (1988). 29. G. Rancoita and A. Seidman, NIM 266, 369 (1984). 30. G. Barbiellini et al, NIM A235, 55 (1985) and E. Borchi et al, CERN-EP/89-28 (1989). 31. M. Oreglia et al, Phys. Rev. D25, 2295 (1982). 32. F. Simon, Nature 135, 763 (1935). 33. Low Temperature Detectors for Neutrinos and Dark Matter, ed. K. Pretzl, N. Schmitz, L. Stodolsky, Springer, Berlin (1987); see also K. Pretzl, Proceedings of "Calorimetry in High Energy Physics" World Scientific, 32 (Lisbon 1999).
Invariant mass of tagged b-jets pairs, above background, for associate t fH production and 1OOfb-1 integrated luminosity. 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).
Calorimetry in Particle Physics: Proceedings of the Tenth International Conference, California, USA 25-29 March 2002 by Ren-Yuan Zhu