Page 370 - Tunable Lasers Handbook
P. 370

330     Norman P.  Barnes

                                      A = 2.33907 + 8.20 X lo-’  (T - 25)
                                      B = 2.58395 -10.47  x lo-’  (T - 25)


                                      C = 0.4588 + 1.13 x 10-5 (T - 25)
                                      D = 13.8169 + 7.73 x lo-’  (T - 25)


                                                E = 519.66


                                     A = 2.35084 - 100.78 X  lo-’  (T - 25)

                                     B = 2.22518 + 114.47 x 10-j (T - 25)

                                      C = 0.04371 - 0.24 X lo-’  (T - 25)

                                     D = 15.9773 - 107.60 x   (T - 25)

                                                E = 741.15


                    for the ordinary and extraordinary Sellmeier refractive indices, respectively. In these
                    expressions, temperature T is given in  degrees centigrade. Operation at  105°C is
                    only a small extrapolation of the refractive index data. taken at 25 and 80°C.
                       In  cases  where  insufficient  data  are  available for  complete temperature-
                    dependent Sellmeier coefficients, the variations of  the  ordinary and  extraordi-
                    nary refractive indices are given for selected wavelengths [35,37,41,4547]. Far
                    from the absorption features of the nonlinear crystal. the variation of the refrac-
                    tive index with temperature is relatively insensitive to the wavelength. Values for
                    the variation of the ordinary and extraordinary refractive index with temperature
                    are tabulated in Table 1.
                       Using the Sellmeier constants listed in Table 5, the phase-matching curves
                    for Type I phase matching have been calculated for the selected uniaxial nonlin-
                    ear crystals listed. For these calculations, pump wavelengths are 0.355, 0.532.
                    1.064, and 2.10 ym. Solid-state lasers make convenient pump sources for optical
                    parametric oscillators because these lasers can operate either in  a cw  or a Q-
                    switched mode. In particular, the Q-switched mode, with its short pulse lengths
                    and concomitant high peak powers, is conducive to the operation of optical para-
                    metric oscillators and amplifiers. Pump lasers operating at these wavelengths can
                    be obtained from a Nd:YAG laser and its harmonics or from either a Ho:Tm:Cr:
                    YAG  or Ho:Tm:Er:YLF laser. Phase-matching curves generated in this manner
                    are not intended to be an exhaustive compilation of  the possibilities but rather
                    are intended to  suggest some of  the  more common situations. Other possible
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