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We extend the existing quasiclassical theory for the superconducting proximity effect in a chaotic quantum dot, to include a time-reversal-symmetry breaking magnetic field. Random-matrix theory (RMT) breaks down once the Ehrenfest time ₄ becomes longer than the mean time ₃ between Andreev reflections. As a consequence, the critical field at which the excitation gap closes drops below the RMT prediction as ₄∕₃ is increased. Our quasiclassical results are supported by comparison with a fully quantum mechanical simulation of a stroboscopic model (the Andreev kicked rotator).
Goorden et al. (Tue,) studied this question.