Page 436 - Tunable Lasers Handbook
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396     Paul Zorabedian













                                                                   !2.0
                                               Wavelength (nm)
                  FIGURE 24  Transmission spectrum of an AOTF driven at 89.139 MHz. (Reproduced with per-
                  mission from Zorabedian [46]. 0 1995 IEEE.)



                  where I, and Id are, respectively, the incident and diffracted intensity, Pa is the
                  acoustic power, h and 1.1’ are, respectively, the height and width of the transducer,
                  and M  is an acousto-optic figure of merit which is -1021  sec3/g for TeO,. A dif-
                  fraction efficiency in excess of  80% has been obtained at 1.3 pm with 5.5 W of
                  rf‘ drive power.

                  7.2.2.2.4  Design Trade-offs
                      The properties of  acousto-optic filters can be tailored to the application by
                  varying the angles of the optical and acoustic beams with respect to the crystal
                  axes. Many  applications of AOTFs are in  spectroscopy and imaging, in  which
                  case  good light-gathering  efficiency requires  that  the  filter have  a  wide  input
                  acceptance angle of several degrees. In contrast, laser tuning applications require
                  narrow bandwidth and high transmission, while on the other hand a field of view
                  of  a  few  tenths  of  a  degree  is  adequate  for  intracavity use.  It  is  beyond  the
                  scope of  this chapter to discuss the design trade-offs of AOTFs  in detail. Some
                  aspects of this topic are discussed in a paper by Booth and Findlay [78]. A com-
                  petent  manufacturer of  AOTFs  will understand these  trade-offs and be able to
                  design an appropriate filter once the requirements are carefully specified.
                  7.2.2.2.5  Frequency Chirp
                      Because  the  incident  light  is  diffracted  by  a  moving  phase  grating,  all
                  AOTFs have the property that the filtered output light  is Doppler  shifted with
                  respect to the input light such that vd = vI k fa, where vd and vI, are, respectively,
                  the  optical frequencies  of  the  diffracted and  incident beams.  The  sign of  the
                  chirp depends on the input polarization and the direction of  propagation. For a
                  given propagation  direction.  e-  and  o-polarized  input  beams  receive opposite
                  chirps. Similarly. reversing the direction of  propagation changes the sign of the
                  chirp  for  a  given  direction  of  propagation.  There  are  two  chirping  and  two
                  dechirping configurations (Fig. 25).
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