Abstract

We explore the one-loop electroweak radiative corrections in the minimal SU(5)SU(5) and the no-scale flipped SU(5)SU(5) supergravity models via explicit calculation of vacuum polarization contributions to the ϵ1,2,3\epsilon_{1,2,3} parameters. Experimentally, ϵ1,2,3\epsilon_{1,2,3} are obtained from a global fit to the LEP observables, and MW/MZM_W/M_Z measurements. We include q2q^2-dependent effects which have been neglected in most previous ``model-independent" analyses of this type. These effects induce a large systematic negative shift on ϵ1,2,3\epsilon_{1,2,3} for light chargino masses (m_{\chi^\pm_1}\lsim70\GeV). In agreement with previous general arguments, we find that for increasingly large sparticle masses, the heavy sector of both models rapidly decouples, \ie, the values for ϵ1,2,3\epsilon_{1,2,3} quickly asymptote to the Standard Model values with a {\it light} Higgs (m_{H_{SM}}\sim100\GeV). Specifically, at present the 90%90\% CL upper limit on the top-quark mass is m_t\lsim175\GeV in the no-scale flipped SU(5)SU(5) supergravity model. These bounds can be strengthened for increasing chargino masses in the 50-100\GeV interval. In particular, for m_t\gsim160\GeV, the Tevatron may be able to probe through gluino(g~\tilde g) and squark(q~\tilde q) production up to m_{\tilde g}\approx m_{\tilde q}\approx250\GeV, exploring at least half of the parameter space in this model.Comment: 15 pages,(6 ps figures available upon request), TeX(harvmac), CTP-TAMU-19/93, ACT-07/9

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