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8  Tunable External-Cavity Semiconductor  Lasers   41 1

                     changing the cavity length. 4s will be shown later, this can be accomplished by
                     AOTFs without the use of moving parts in the cavity.


                     10.2  Embodiments of Phase-Continuous Tuning
                        Phase-continuous tuning over a 15-nm range was obtained without senlocon-
                     trol from a  1.26-pm Liatrow-grating-tuned extended-cavity laser using  a rather
                     complex mechanical arrangement in  which  the  grating was mounted  on  a bar
                     whose ends were pinned to a pair of  orthogonal sliding stages [107]. It is also
                     possible to achieve continuous tuning with  a single mechanical degree of  free-
                     doni. Phase-continuous tuning over a range of  1000 GHz wa5 obtained by push-
                     ing with a PZT on a pivot arm that simultaneously rotates and translates the grat-
                     ing [lo81 (Fig. 36). Up to 82 nm  (more than  10.000 GHz) of  phase-continuous
                     tuning has been reported [ 1091. The grating is mounted on a pivot arm, which is
                     rotated about an axis lying near the intersection of  the grating surface and  the
                     plane  of  the  laser diode output facet. The mode-hop-free tuning range is quite
                     sensitive to the precise location of  the rotation axis  (Fig. 37). There have been
                     several studies of  the optimum location of  this "magic" pivot point, taking into
                     account chromatic dispersion and  phase  shifts introduced by  the  gain medium
                     and various intracavity optical elements [ 110-1 131.
                        Phase-continuous tuning can also be realized with an acousto-optically con-
                     trolled ECL. Introducing a slight offset (e.g.. -1  Hz) between the drive frequen-
                     cies of the two intracavity filters will generate a net chirp of the oscillating mode
                     on each round-trip. If  the passbands of  the filters are simultaneously slewed so
                     as to match  the  induced chirp. phase-continuous tuning will result  [114]. The
                     key to the success of this method is to obtain single-mode oscillation in the first
                     place, which is difficult because of the broad bandwidth of AOTFs.


                                                Axis of















                                       output'
                                       coupling lens   k=2cmi
                     FIGURE  3 '6  Phase-continuous  tuned grating extended-cavity  laser with PZT actuator. (Repro-
                     duced with permission from Schremer and Tang [lo@. 0 1990 IEEE.)
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