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note
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The theoretical cuve of group delay versus frequency (see Fig. 1; see also solid curve in Fig. 4) shows that, for a pulse with a carrier frequency ω far from the two resonance peaks by a few times the Lorentzian width, the group delay approaches zero, which means that in Fig. 1, ΔL ≃ 0. Off-resonance pulses are thus reflected close to the entrance plane of the FBG structure, thus providing an important reference in the experimental measurements.
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