Page 292 - Fiber Bragg Gratings
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6.5 The optical circulator based OADM                           269

         edges of the reflection band (see Chapter 4). If the signal fills the grating
         or is severely limited by the grating bandwidth, apart from the simple
         pulse broadening (narrowed spectrum), additional dispersion from the
         band edges of the grating has the potential of causing severe pulse distor-
         tion. This area has only recently received attention [631.
             Programmability of an OADM is often desirable, and there are several
         techniques available to integrate this feature. As has been seen with
         the GMZI-BPF, the most easily adjustable parameter is the path length
         difference from the coupler to the gratings, since tuning the Bragg wave-
         length of both gratings poses a difficult engineering problem. The OC-
        ADM is not an interferometric device, so that tuning of the gratings by
         stretching/compressing or heating is easily achieved. Quetel et al. [651
         demonstrated this principle with a circulator and four gratings stretch
        tuned by piezoelectric (PZT) actuators, with a switching time of 40 ytts
         and a voltage of only 50 V. Okayama et al. [64] proposed the use of a pair
         of identical gratings for each add/drop channel with two 4-port optical
         circulators for an OC-based tunable add-drop multiplexer (OC-TADM).
        Figure 6.34 shows the arrangement of the gratings for a four-channel
         OC-TADM. Channels arriving at the input port are reflected by the appro-
        priate gratings, A 1? A 2, A 4 in the top part of the circulator branch, group
         1. Gratings 2 and 4 are tunable (by either temperature or strain); however,
         all channels are reflected and routed to the second set of gratings, A 4, A 2,
         A 2, Aj in the bottom part of the circulator branch, group 2. In this section,
        gratings 3 and 1 are tunable. If each grating pair has identical Bragg
        wavelengths, all channels are routed to the drop port by reflections from
        group 2 gratings. However, since one of the gratings of the matched pair



















        Figure 6.34: Dynamic wavelength selective add/drop mux-demux using tun-
        able gratings (after Ref. [64]).
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