Page 415 - Tunable Lasers Handbook
P. 415

8  Tunable External-Cavity Semiconductor  Lasers   375

                     media or by going to tapered-stripe gain media. Recently, up to -lW  output has
                     been  obtained from  an external cavity laser  with  a tapered-stripe  gain medium
                     [43]. The  output  beam  was  described  as  diffraction-limited. The  coupling  effi-
                     ciency to optical fiber was not reported.



                     5. FEEDBACK MODEL

                     5.1  Effective Reflectance
                         The basic model  for  an  extended-cavity laser is  based  on a  3-mirror com-
                     pound  cavity  (Fig.  11). The  interior facet of  the gain medium  and the external
                     reflector foorm  a compound mirror. This compound mirror together with the out-
                     side facet form a Fabry-Perot  resonator. The effective reflectance of the extended
                     cavity, including multiple reflections from the inside facet, is given by [43]







                     In  a  double-ended  external  cavity.  each  extended-cavity  section  has  its  own
                     effective reflectance. ~e.,








                     where i denotes extended-cavity section 1 or 2. The various parameters are defined
                     in Table 4. The external feedback in a ring cavity is characterized by a wavelength-
                     dependent coupling strength c&)   which gives the fraction of the field amplitude
                     from facet 1 that is coupled into facet 2. In the absence of nonreciprocal intracavity

















                                   FIGURE  1 4 Extended-cavity laser feedback model.
   410   411   412   413   414   415   416   417   418   419   420