Physics – High Energy Physics – High Energy Physics - Phenomenology
Scientific paper
2003-06-30
Eur.Phys.J. C34 (2004) 157-163
Physics
High Energy Physics
High Energy Physics - Phenomenology
18 pages, latex, 8 figures (version to appear in EPJC)
Scientific paper
10.1140/epjc/s2004-01668-9
Heavy charged Higgs bosons ($H^\pm$) of a Type II 2-Higgs Doublet Model (2HDM) can be detected at future electron-positron Linear Colliders (LCs) even when their mass is larger than half the collider energy. The single Higgs mode $e^+e^-\to t\bar b H^- + ~{\rm{c.c.}} \to 4b +{\rm{j}}{\rm{j}} + \ell + p_T^{\rm{miss}}$ (where j represents a jet and with $\ell=e,\mu$) contributes to extend the discovery reach of $H^\pm$ states into the mass region $M_{H^\pm}\gsim \sqrt s/2$, where the well studied pair production channel $e^+e^-\to H^-H^+$ is no longer available. With a technique that allows one to reconstruct the neutrino four-momentum in the decay $t\to b W^+\to b \ell^+\nu$, one can suppress the initially overwhelming main irreducible background due to $e^+e^-\to t\bar t b\bar b$ (via a gluon splitting into $b\bar b$ pairs) to a negligible level. However, for currently foreseen luminosities, one can establish a statistically significant $H^\pm$ signal only over a rather limited mass region, of 20 GeV or so, beyond $M_{H^\pm}\approx \sqrt s/2$, for very large or very small values of $\tan\beta$ and provided high $b$-tagging efficiency can be achieved.
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