The minimal supersymmetric extension of the standard model (MSSM) is the simplest realistic SUSY theory. The Higgs sector in the MSSM consists of two charged and three neutral scalar bosons. Assuming CP-invariance, one of the neutral bosons (A) is CP-odd, and the other two (h,H) are CP-even. Here we use h (H) for the lighter (heavier) CP-even neutral Higgs boson, and φ to denote any of h,H,A. At tree level, the MSSM Higgs bosons are described by the mass of A (mA), and tanβ=vu/vd, where vu, vd are the vacuum expectation values of the neutral Higgs fields that couple to up-type and down-type fermions, respectively. The Yukawa couplings of A to down-type fermions are enhanced by a factor of tanβ relative to the SM. For large tanβ one of the CP-even bosons is nearly mass-degenerate with A and has similar couplings. The dominant production mechanisms of neutral MSSM Higgs bosons at hadron colliders are gluon fusion and bb fusion. The leading decay modes of A and the corresponding mass-degenerate CP-even Higgs boson are φ → bb (~90%) and φ→ττ (~10%).

Radiative corrections can significantly modify the MSSM Higgs production cross sections and branching fractions, and introduce dependence on additional model parameters. The results are usually interpreted in predefined "benchmark scenarios" that serve as representative points in the (large) SUSY parameter space. Information on generaly used benchmark scenarios can be found in Carena et al. (1999) and Carena et al. (2002). The authors of these papers have produced an updated and very comprehensive review of the treatment of radiative corrections in the MSSM Higgs sector: M. Carena, S. Heinemeyer, C.E.M. Wagner, and G. Weiglein, hep-ph/0511023 (2005). In my opinion this is one of the "must read" papers for any experimentalist working in the field.

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Last update 12/08/2005