Page 312 - Tunable Lasers Handbook
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272     Norman P.  Barnes

                  lower, which limits the average power available from these laser materials. Some
                  of the physical properties of these laser materials are listed in Table 5.
                      Garnet  materials  are  isotropic  materials  with  a  relatively  high  refractive
                  index. As expected, the refractive index of  these materials is higher than that of
                  YAG. Specifically, the refractive indices of GSGG, YSAG, and GSAG are 1.952,
                   1.867, and 1.890, respectively. Because these materials are isotropic, laser output
                  is not polarized in general. If polarizers are included in the laser resonator. depo-
                  larization losses can be expected at high average powers [47,48]. Depolarization
                  losses are due to the thermally induced birefringence in normally isotropic mate-
                  rials and are exacerbated by  the reduced thermal conductivity when compared
                  to YAG.
                      When Cr is incorporated into these materials, the two absorption bands char-
                  acteristic of Cr are readily identified. Absorption peaks for the short-wavelength
                  absorption are approximately 1.5 times stronger than the absorption peaks for the
                  long wavelength. Spectra of Cr:GSGG and Cr:GSAG appear in Figs. 24 and 25,
                  respectively.  Short-wavelength absorption  peaks  occur  at  0.46  and  0.45  pm:
                  widths are 0.09 and 0.12 pm for GSGG and GSAG, respectively [49,50]. Long-
                  wavelength absorption peaks occur at 0.64 and 0.63 pm; widths are 0.12 and 0.09
                  pm for the same laser materials. These absorption features are strong enough to
                  produce  absorption coefficients on the  order of  200 m-1  even with concentra-
                  tions  below  0.01  atomic.  Efficient  flashlamp pumping  is  possible  with  these
                  materials  because  of  these  strong  absorption  features.  However,  the  shorter
                   wavelengths, shorter than about 0.4 pm, should be filtered out since these wave-
                  lengths  are  absorbed primarily by  the laser material  itself. Short pump  wave-
                   lengths thus  contribute to  heating  of  the  laser  material  while producing  little
                  population  in  the  upper  laser  level. Worse  still  is  the  creation  of  detrimental
                  flashlamp-induced loss.





                  TABLE  5  Physical Properties of Garnets

                                                                    ~~
                   Parameter              YAG            GSGG              Units
                   Lattice constants      1201            1256
                   Density                4550            6439
                   Heat capacity           620            402
                   Thermal conductivity     13.0            5.78
                   Thermal expansion        7.0             7.5
                   Refractive index         1.8289          1.9518
                   Refractive index variation   10.4       10.1              10-6K
                   Optical transparency     0.24-5.5        0.3-6.5          Pm
                   h1elting point         1940           ~1830               "C
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