By Abe, T
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Additional resources for Linear Collider Physics Resource Book for Snowmass 2001, 2: Higgs and Supersymmetry Studies
Using neural net tags and full kinematic fitting , the mass peak shown in Fig. 18(b) is obtained for mhSM = 120 GeV, √ s = 500 GeV, and 500 fb−1 resulting in ∆mhSM ≃ 50 MeV. If a second lower-energy IR is available, it might be attractive to perform a scan across the Zh threshold. With a total integrated luminosity of 100 fb−1 , ∆mhSM ≃ 100 MeV at mhSM = 150 GeV is achievable , competitive with the methods above. 18: (a) Jet-jet invariant mass of the jets recoiling from a Z reconstructed hadronically simulated in the LCD Large detector, mhSM = 115 GeV.
Under such conditions, one can precisely measure the recoil mass in e+ e− → Zh events opposite to the reconstructed leptonic decay Z → e+ e− or µ+ µ− . This measurement is independent of the Higgs decay mode. Accuracy can be improved by reconstructing specific decay modes, leading, for example, to a four-jet topology where effective (5-C) kinematic constrained fits can be employed. 12) in a simulation of the L linear collider detector  described in Chapter 15 for Higgs masses between 115 and 160 GeV .
A comprehensive description of European studies using the simulated TESLA detector can be found in . North American studies consider simulations of detectors with capabilities described in Chapter 15. The program of measurements of Higgs boson properties strongly impacts detector design. Measurement of branching ratios into fermions requires sophisticated vertex detectors to separate b from c (and gluon) jets. Precise recoil mass measurements need excellent momentum resolution (particularly for µ+ µ− ) from charged particle tracking.