“…In this case, relation ( 5) is modified to (9) The extra jitter due to AM, denoted as , enters time relationship (6) as follows 1 (10) Since in (10) , the first term on the right hand side of ( 9) is well approximated by (11) The error introduced by this approximation is of the order of and thus it is negligible compared to . Thus, plugging (11) into ( 9) and exploiting the -periodicity of and of , we obtain (12) In Section IV, it will be proven that, for a harmonic interference, the amplitude waveform takes the form (13) where is a -periodic function (i.e., an element of a Floquet eigenvector) while is a slowly-varying coefficient oscillating with frequency . In this case, using the approximation and the periodicity of , the numerator of ( 12) can be simplified to (14) With this simplification, AM-induced period variation ( 12) is estimated by (15) where is the ratio of over at the crossing time point , which is almost constant over all cycles.…”