Single Dilepton Production at $e^+e^-$, $eγ$ and $γγ$ Colliders

Details Single Dilepton Production at $e^+e^-$, $eγ$ and $γγ$ Colliders Single Dilepton Production at $e^+e^-$, $eγ$ and $γγ$ Colliders

1994-03-07

arxiv.org/abs/hep-ph/9403237v1

Phys.Rev. D50 (1994) 2031-2036

Physics

High Energy Physics

High Energy Physics - Phenomenology

plain TeX, 9 pages + 13 figures (not included, but available upon request), UdeM-LPN-TH-94-190, McGill-94/12

Scientific paper

10.1103/PhysRevD.50.2031

We calculate the cross sections for the single production of doubly-charged dileptons, both scalar and vector, at $e^+e^-$, $e\gamma$ and $\gamma\gamma$ colliders at $\sqrt{s}=500$ GeV and 1 TeV. The $e\gamma$ mode is by far the most promising -- dileptons whose coupling is as weak as $O(10^{-4})\alpha_{em}$ can be observed, for masses virtually up to the kinematic limit. Dileptons of mass up to $\sqrt{s}$ can also be seen in $e^+e^-$ and $\gamma\gamma$ colliders, for couplings of order $\alpha_{em}$. In all three colliders, most of the cross section comes from events in which the only particles detected are $e^-e^-$, the decay products of the dilepton, yielding an unmistakeable experimental signature.

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