Higgs signals and hard photons via $WW$-fusion in the Standard Model at the Next Linear Collider

Details Higgs signals and hard photons via $WW$-fusion in the Standard Model at the Next Linear Collider Higgs signals and hard photons via $WW$-fusion in the Standard Model at the Next Linear Collider

1996-06-07

arxiv.org/abs/hep-ph/9606268v1

J.Phys.G22:1611-1632,1996

Physics

High Energy Physics

High Energy Physics - Phenomenology

27 pages, LaTeX, 10 PostScript figures embedded using epsfig, 8 figures bitmapped at 100dpi, complete paper with higher resolu

Scientific paper

10.1088/0954-3899/22/11/009

Within the framework of the Standard Model, integrated and differential distributions are given for Higgs production via the $WW$-fusion mechanism and decay via the channels $H\ar b\bar b$ and $H\ar WW\ar {jjjj}$, with and without photon radiation, at Next Linear Collider energies. Calculations are carried out at tree-level and rates of the leading processes $e^+e^-\ar\bar\nu_e\nu_e H \ar \bar\nu_e\nu_e b\bar b $ and $e^+e^-\ar\bar\nu_e\nu_e H \ar \bar\nu_e\nu_e WW \ar \bar\nu_e\nu_e {jjjj}$ are compared to those of the next-to-leading reactions $e^+e^-\ar\bar\nu_e\nu_e H (\gamma)\ar \bar\nu_e\nu_e b\bar b \gamma$ and $e^+e^-\ar\bar\nu_e\nu_e H (\gamma)\ar \bar\nu_e\nu_e WW (\gamma) \ar \bar\nu_e\nu_e {jjjj}\gamma$, in the case of hard and detectable photons. Finally, a brief discussion concerning the case of $H\ar ZZ\ar{jjjj} (\gamma)$ decays is also given.

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