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Signal and background for H _ ZZ _ ¢+e-('+£ -. 2-21 2-22 2-23 2-13 2-14 2-15 2-16 2-17 Signal and background for H _ ZZ _ e + e-v_ ............................... Signal and background for H -* ZZ -* _ + e -jj ................................. Jet rates for various substructure scales and parton distributions .................... Effect of weighting schemes on jet substructure................................. Supersymmetry models .................................................... 2-24 2- 26 2-37 2-38 2-49 Chapter 3 3-1 3-2 3-3 3-4 3-5 3-6 3-7 3-8 3-9 Major magnet design options................................................

Lane, Nucl. Phys. B343, 554 (1990). 17. See G. t' Hooft in Reference 8. I INTRODUCTION The GEM collaboration we have taken care to provide the robustness needed was formed in to do the physics that requires high luminosity. June 1991 to develop a major detector for the SSC. The primary physics objectives of GEM are those central to the motivation for the SSC: to study high Pr physics--exemplified by the search for Higgs bosonsDand to search for new physics beyond the standard model, We present in this Technical Design Report (TDR) a detector with broad capabilities for the discovery and subsequent study of electroweak symmetry breaking, the origin of mass and flavor, and other physics requiringprecise measurements of gammas, electrons, and muons--hence the name, GEM.

77'eX ........................................... Signal and background for H --* ZZ" _ _ +e - ¢ +e -. Signal and background for H _ ZZ _ ¢+e-('+£ -. 2-21 2-22 2-23 2-13 2-14 2-15 2-16 2-17 Signal and background for H _ ZZ _ e + e-v_ ............................... Signal and background for H -* ZZ -* _ + e -jj ................................. Jet rates for various substructure scales and parton distributions .................... Effect of weighting schemes on jet substructure.................................

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