Higgs Boson Physics in the $s$-channel at $μ^+μ^-$ Colliders

Details Higgs Boson Physics in the $s$-channel at $μ^+μ^-$ Colliders Higgs Boson Physics in the $s$-channel at $μ^+μ^-$ Colliders

1996-02-27

arxiv.org/abs/hep-ph/9602415v1

Phys.Rept.286:1-51,1997

Physics

High Energy Physics

High Energy Physics - Phenomenology

87 pages, uuencoded tex file and postscript figure files submitted, full postscript file, including embedded figures, is avail

Scientific paper

10.1016/S0370-1573(96)00041-5

Techniques and strategies for discovering and measuring the properties of Higgs bosons via $s$-channel production at a $\mu^+\mu^-$ collider, and the associated requirements for the machine and detector, are discussed in detail. The unique feature of $s$-channel production is that, with good energy resolution, the mass, total width and partial widths of a Higgs boson can be directly measured with remarkable accuracy in most cases. For the expected machine parameters and luminosity the Standard Model (SM) Higgs boson $\hsm$, with mass $\lsim 2\mw$, the light $\hl$ of the minimal supersymmetric Standard Model (MSSM), and the heavier MSSM Higgs bosons (the CP-odd $\ha$ and the CP-even $\hh$) can all be studied in the $s$-channel, with the heavier states accessible up to the maximal $\sqrt s$ over a large fraction of the MSSM parameter space. In addition, it may be possible to discover the $\ha$ and $\hh$ by running the collider at full energy and observing excess events in the bremsstrahlung tail at lower energy. The integrated luminosity, beam resolution and machine/detector features required to distinguish between the $\hsm$ and $\hl$ are delineated.

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