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Because of the large number of adjoint fields $N_A$ coupled to S, one finds that M can be generically close to $M_{GUT} = 2 \\times 10^{16} GeV$:\n  $M \\simeq M_{Pl} \\exp[-16 \\pi^2 \\log(3/2) / (N_A+4) \\lambda^2]$, where $\\lambda$ is a Yukawa $\\sim$ 0.7. 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