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As can be seen, the concept of recovery time was somewhat generalized here. Usually the medium is perturbed by a wave which has the same amplitude as the wave emitted after the perturbation. These "self"-recovery times R(L → L) and R(H → H) exhibited no asymmetry in contrast with the "cross"-recovery times R(L → H) and R(H → L). It is rather probable that R(H → L) = R(L → L). This is because R(H → L) cannot be shorter than R(L → L) otherwise waves crossing the HL boundary would not be able to propagate in L. On the other hand, regarding the high amplitude of the incoming wave, R(H → L) cannot be longer than R(L → L) either. Thus, all recovery times are roughly equal except R(L → H) which is considerably longer than the others.
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