Page 399 - Tunable Lasers Handbook
P. 399

8  Tunable External-Cavity Semiconductor  Lasers   359

                               oxide-              -contact        Gain guided
                             cladding<<            - active layer   narrow stripe





                              oxide - 1            -contact





                              oxide -              -contact       Index guided

                             cladding4             -active   layer   ridge waveguide


                        FIGURE 5  Schematic diode laser cross sections showing common waveguide structures



                     2.6.3  lateral Guiding Structures
                         Lateral optical guiding  is necessary to confine the radiation ta  the region of
                     the diode possessing optical gain. There are three basic types of guiding structures
                     (Fig. 5): gain guiding, strong index guiding, and ridge guiding. which utilizes both
                     gain and index guiding. The reader is cautioned that these illustrations are highly
                     schematic and are only intended to convey the basic structure. For more detailed
                     treatment  of  semiconductor  laser  structure.  see,  for  example,  Ref.  [lo]. Brief
                     descriptions,  of these structures follow.

                     2.6.3.1  Gain-Guided Oxide Stripe Devices
                        In this type of laser, current is injected through a narrow (5 to 10 pm wide)
                     opening in the top dielectric layer. Gain is laterally confined to the region around
                     the stripe by the limited lateral diffusion of carriers. The region beyond the stripe
                     exhibits large absorption losses, and so light is laterally confined to the region of
                     the pumping stripe even though there is no refractive index profile. The emitting
                     spot is approximately 1 x 10 pm.
                         Gain-guided devices are easy to fabricate and are therefore often used to test
                     semiconductor material quality. However, they suffer from three disadvantages:
                     (1 j Because of the high absorption losses, they have a high threshold current. (2)
                     The  spot  size  and  divergence  are  dependent  on  the  pumping  current.  Higher
                     order transverse modes may appear at high current. (3) Because there is no lat-
                     eral index profile, gain-guided lasers have from 5 to 50 pm of astigmatism.
   394   395   396   397   398   399   400   401   402   403   404