Page 368 - Tunable Lasers Handbook
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328     Norman P.  Barnes

                       AgGaSe,  has large nonlinear coefficients but suffered initially from limited
                   transmission%  the near infrared. Absorption in the near infrared has been miti-
                   gated to a large extent by an annealing process. Because of the large vapor pres-
                   sure  of  Se.  this  material  often  grows  Se  deficient.  To  overcome  this,  grown
                   crystals have been annealed in Se-rich atmospheres. By doing this, the absorp-
                   tion in the near infrared is substantially reduced. Birefringence of this material
                   is sufficient to effect phase matching but not so large as to impose severe accep-
                   tance  angle problems.  Both  optical parametric  oscillators  and amplifiers have
                   been demonstrated using this material.
                       ZnGeP,  has  an even larger nonlinearity than AgGaSe,.  It too suffers from
                   absorption problems in the near infrared. As this material has a high vapor pres-
                   sure during  growth, an  absorption  analogy  with AgGaSe,  is possible.  Several
                   approaches to lowering this absorption have been tried with varying degrees of
                   success. Birefringence of  this material allows phase matching of  a wide variety
                   of  nonlinearity  interactions  without  incurring  severe birefringence  effects.  In
                   addition, this material has better thermal characteristics than AgGaSe,.
                       TAS, or T13AsSe,,  is  a mid-infrared nonlinear crystal with  sufficient bire-
                   fringence to allow phase matching of  a wide variety of nonlinear interactions. It
                   has reasonably large nonlinear coefficients that have allowed its use as a nonlin-
                   ear crystal. However, as mid-infrared nonlinear crystals with even larger nonlin-
                   ear coefficients are available. this material also has seen somewhat limited use.

                    8.  PHASE-MATCHING CALCULATIONS

                       Phase-matching curves are used to describe the orientation of the nonlinear
                   crystal for which phase matching will be achieved. In uniaxial crystals. the angle
                   for which phase matching is achieved is usually displayed as a function of  the
                   interacting wavelengths. In biaxial crystals, two  angles are needed to  describe
                   the orientation  of  the  nonlinear  crystal. Consequently, phase  matching  can be
                   achieved at a locus of  points. Thus. for a given set of  interacting wavelengths.
                   the locus of the phase matching angles is usually described in terms of the polar
                    and  azimuthal  angles.  To  determine  the  phase-matching  angle  or  angles.  the
                   refractive indices at the interacting wavelengths must be determined.
                       A Sellmeier equation can be used to describe the variation of the refractive
                   indices  with  wavelength.  Historically  several  equations  have  been  used  to
                    describe the variation of  the refractive index as a function of  wavelength. How-
                    ever, the Sellmeier equation has  several advantages, including a physical basis
                    and the ability to describe  accurately the refractive index over relatively large
                   wavelength  intervals.  Several  forms  of  the  Sellmeier  equation  have  been
                   reported, but the  form that is most usually associated with a physical basis is
                    expressed as
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