Page 407 - Tunable Lasers Handbook
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8  Tunable External-Cavity Semiconductor  Lasers   367
                     where nl and tl are the index and thickness, respectively. of the lnner layer and
                     n, and t, are the index and thickness, respectively, of  the outer layer. This prin-
                     ciple can be extended to three layers by incorporating a third quarter-wave layer
                     with an intermediate index of refraction tz3 = no (iznJn0)~ between the two layers
                     specified above.  Other  index  and  thickness  combinations  for  two-  and  three-
                     layer antireflection coatings are also possible.
                         Antireflection coatings with three dielectric layers in a low-high-low  sequence
                     of  refractive indices have been used to relax the tolerances and broaden the low-
                     reflectance banda idth [29,30].

                     2.10.2.3 Antireflection Coating Materials
                         The most widely used material for antireflection coatings on AlGaAs and
                     InGaAsP facets is nonstoichiometric  SiOl, which can be deposited by thermal
                     [25] or electron-beam  evaporation  [31]. The composition  and  the  film  index
                     can  be  adjusted  by  varying  the  oxygen  pressure  in  the  deposition  chamber.
                     Sputtered  Si3N, films have  also been  used  on  0.85-ym AlGaAs  and  1.3 and
                     1.55 ym  InGaAsP  laser  diodes.  resulting  in facet reflectances  in the  0.01 to
                     0.03% range [32].

                     2.7 0.3  Passivation Layers
                         Commercial telecommunication and CD laser diodes are often shipped with
                     h/2 hcet passivation layers. It is possible to etch off the passivation layer prior to
                     coating or to deposit the antireflection coating over the passivation layer, but it is
                     preferable to start with unpassivated devices if possible.
                     2.7 0.4 Angled Facets
                         4n alternative to antireflection coatings is to use an optical amplifier with an
                     angled gain stripe in an external or ring cavity. The waveguide is slanted from
                     the cleavage plane  so that  the  internal Fresnel reflection  from  the  facet is not
                     coupled back into the waveguide and lost. The effective reflectance of the lonest
                     order TE mode decreases exponentially with the slant angle [33]. However. the
                     reflectance of the higher modes increases with the slant angle. Therefore. caution
                     must be  exercised if  the stripe is wide enough to  support higher order modes.
                     For a 2-ym  stripe, the calculated facet reflectance is on the order of  10-3  for a
                     slant angle of  10" [31].
                         Even though the internal facet reflections do not couple back to the wave-
                     guide. there are still reflections at the semiconductor-air  interface that represent
                     loss  in  coupling  to  the  external  cavity. The  coupling  loss can  be  redwed  by
                     applying antireflection coatings to the angled facets [35].

                     2. 70.5 Buried Facets
                         Another means of  facet reflectance reduction is the use of  gain media with
                     buried facets  [36]. In  these devices the waveguide stops several microns inside
                     the  chip,  with  semi-insulating material  between  the  end  of  the  guide  and  the
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