Page 377 - Tunable Lasers Handbook
P. 377

7 Optical Parametric OsciIIators   337

                                    12.0
                                    11.0
                                    10.0
                                 h
                                  $  9.0
                                  +
                                  a,
                                  E  8.0
                                  e
                                  .- E  7.0
                                  v
                                  5  6.0
                                  0,
                                  C
                                  2 5.0
                                  a,
                                  >
                                  3  4.0
                                     3.0
                                     2.0
                                     1 .o
                                               I       I      I       I
                                       30      32     34      36      38
                                                 Angle (degrees)
                              FIGURE  1 8  Phase-matching cune for AgGaS,  for a 2.10-pn pump


                     lasers.  Both  increased  beam  quality  and  decreased  linewidth  can  lead  to  an
                     increased performance for the optical parametric oscillator.
                         Several different concepts are involved in the assessment of the performance
                     of an optical parametric oscillator including threshold, slope efficiency, total effi-
                     ciency. photon efficiency, and pump depletion. Optical parametric oscillators can
                     be operated either in a cw or a pulsed mode. Of the two modes of operation. the
                     pulsed mode is much more common since the operation of an optical parametric
                     oscillator is enhanced by a high power density. The threshold in the cwr mode is
                     straightforward to define as the amount of pump power required to achieve opti-
                     cal parametric oscillation. In the pulsed mode.  the observable threshold, rather
                     than the instantaneous threshold. is usually  quoted; however. this is not alw ays
                     made clear. While slope efficiency is sometimes quoted, it could represent either
                     the  ratio  of  the  increase  in  power  at the  output  wavelength  to  the  increase  in
                     power  at the pump wavelength or the increase in power  of  both the  signal and
                     idler wavelengths to the increase in power at the pump wavelength. In the pulsed
                     mode. it could be quoted at the instant of peak power or it could be quoted for the
                     total output energy. Although laser theory usually predicts a nearly linear increase
                     in the output with increases in the input. optical parametric oscillator theory does
                     not  necessarily  predict  the  same  approximation. However, in  practice.  a  linear
   372   373   374   375   376   377   378   379   380   381   382