Page 333 - Tunable Lasers Handbook
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Norman P.  Barnes
                                   NASA Langle!  Research Center-
                                   Hanipton. I i'rginia






















                     I.  INTRODUCTION

                        Optical parametric  oscillators are a  convenient  method  to  create  a  widely
                     tunable sour'ce of laser radiation. An optical parametric oscillator begins with a
                     pump  laser.  In  many  cases  the  pump laser  is  a  well-behaved  solid-state laser
                     such as a Ndl:YAG laser or a frequency-doubled Nd:YAG  laser. To complete the
                     system,  a nonlinear  crystal between  a  set of  mirrors  is required. As  such, the
                     optical parametric  oscillator by  itself  is an  extremely  simple device.  Using an
                     optical parametric oscillator, any wavelength  longer than the pump wavelength
                     and nominally within the transparency region of the nonlinear crystal can be cre-
                     ated. However. practical  problems  limit the range of  generated wavelengths  to
                     those that are somewhat longer than the pump wavelength, nominally a factor of
                     1.2 or so.
                        Optical parametric oscillators may be regarded as photon splitters. That is, a
                     pump photon is split into two photons or one photon divides itself to create two
                     photons. To satisfy conservation of energy, the sum of the energy of the two cre-
                     ated photons  must equal the energy of the pump photon.  With the energy of  a
                     photon given by hv where  12  is Planck's  constant and v  is the frequency of the
                     photon, the conservation of energy can be written as



                     Timohle Laser-s Hrmdhmk
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