Equations (A·16), (A·18) and (A·20) in the Appendix should read (A·16)(A·18)(A·20) Our nnumerical results for large Yukawa couplings are slightly affected by the above correction. However, the essential feature of the paper is unchanged. Especially the lower bound on the top quark mass in our scenario (~60 GeV) is not sensible affected.
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Inoue et al. (1983) studied this question.