Dilepton Production in $e^- p$ and $e^+ e^-$ Colliders

Details Dilepton Production in $e^- p$ and $e^+ e^-$ Colliders Dilepton Production in $e^- p$ and $e^+ e^-$ Colliders

1992-06-23

arxiv.org/abs/hep-ph/9206244v1

Nucl.Phys. B386 (1992) 267-279

Physics

High Energy Physics

High Energy Physics - Phenomenology

16 pages, 3 figures (not included), IFP-428-UNC

Scientific paper

10.1016/0550-3213(92)90567-U

In an $e^- p$ collider, a striking signature for a dilepton gauge boson is \ep \ ; this cross-section is calculated by using the helicity amplitude technique. At HERA, with center-of-mass energy $\sqrt s = 314 GeV$, a dilepton mass above $150 GeV$ is inaccessible but at LEPII-LHC, with a center-of-mass energy $\sqrt s = 1790 GeV $, masses up to 650 GeV can be discovered. In an $e^+ e^-$ collider, the signature is \ee \ . The cross-sections of this process are also calculated for the center-of-mass energies $\sqrt s = 200, 500$ and $1000 GeV$.

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