Page 192 - Instrumentation Reference Book 3E
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176  Fiber ootics in sensor instrumentation
             Broad-Band
               Source
            (Fiber Coupled)
                       6                    Reflected Light   Path Imbalance
                                                            S
              (Coherence                    4-          Optical Sensing
                                                         Interferometer
                             Optical Processing
                                                            L >> IC
                             Interferometer Path
                              Imbalance within
                                 L f I$




                              Electronic Decoding
                                    Unit              (a)



















                                                      (b)
            Figure 12.6   (a) Basic configuration of a"white4ght" interferometric sensor system using two coupled interferometers.
            (b) Output temporal fringe pattern (lower trace) from a"white-light" interferometric sensor system using PZTsawtooth
            displacement ramp of Xi2 (upper trace) (Meggitt 1991).
            linearly displaced over 1 wavelength range (with   interferometry this  factor  is usually between  1/2
            fast  flyback)  such  that  the  output  interference   and 1/3 in fringe modulation depth. It is seen that
            pattern  is  driven  over  one  complete  interfero-   the  phase  of  the  cosine fringes is  a  function  of
            metric  fringe, as shown in Figure  12.6(b) (Meg-   the path difference between the imbalance of the
            gitt  1991). The  phase  of  this  induced  carrier   sensing and  reference  interferometers. Since  the
            signal is  then  modulated  by  optical  path length   coherence length of a low coherence source is typ-
            changes in the sensing interferometer in response   ically between 20  and  50pm, it  is  seen that  the
            to changes in the measurand field. The character-   interferometer imbalance in the sensor can be less
            istic equation of the processing system is then:   than  0.1 mm  and,  therefore,  represents  a  near
                                                      point sensing device. In addition, it is the differ-
                                                      ence in  the path  length  imbalance  between  the
                                                      two  interferometers  that  is  sensitive to  fluctu-
                                                      ations in the source central wavelength. This quan-
                         47r(nL, -nLz)        (12.5)   tity  will  necessarily  be  less  than  the  coherence
                     w,t-                             length of the source (<100p,m) and typically less
                              A,
                                                      than  10pm. Therefore, it is seen that, compared
            where cr  represents  the  half-width  of  the  source   with  the  wavelength  modulated  pseudo-hetero-
            spectrum at which the optical power falls to lle of   dyne  laser  diode technique,  the  wavelength  sta-
            its maximum value at k,,  and w,  is the induced   bility  requirements  will  be  in  the  ratio  of  their
            carrier  signal.  The  exponential  term  represents   respective cavity imbalances, that is; < 1000 times.
            the  visibility  of  the  fringes  and  in  white-light   It is this factor that has largely been responsible
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