Page 107 - Photodetection and Measurement - Maximizing Performance in Optical Systems
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System Noise and Synchronous Detection

            100   Chapter Five

                            -50
                                                  1172Hz
                            -60
                                      1100Hz          1200Hz          1300Hz
                         Voltage (dBm)  -70                   1250Hz


                            -80


                            -90              1150Hz

                           -100
                              1050    1100     1150    1200     1250    1300     1350
                                                   Frequency (Hz)
                        Figure 5.6 Positioning the modulation frequency (1172 Hz) between the interfering
                        harmonics can greatly improve S/N measurement. Hitting a harmonic would
                        degrade S/N by about 25 dB.


                        modulate at the “right” frequency. This might mean accurately between two
                        harmonics of 50/60Hz. Figure 5.6 shows an expanded spectral analysis cover-
                        ing 1050 to 1350Hz. The 1100Hz, 1200Hz, 1300Hz room-light harmonics are
                        evident, as well as vestiges of 50Hz harmonics. The modulated source signal
                        has been deliberately placed between two harmonics, in this case at a frequency
                        of 1172Hz. If the modulation had been chosen instead at 1200Hz, on top of a
                        strong harmonic, the measurement S/N would have been degraded by at least
                        25dB, perhaps the difference between a reasonable measurement and a failed
                        experiment. Not only is the S/N greatly reduced by measuring on a disturbing
                        harmonic, but if the reference clock drifts in frequency, the interference mag-
                        nitude will change with time. This variable behavior can make diagnosis of
                        intermittent poor S/N problems very difficult.
                          The only sound way to choose the frequency is to first investigate the fre-
                        quency spectrum of the optical receiver’s output. This can be done using a
                        conventional electronic spectrum analyzer, by using the Fourier transform algo-
                        rithms built into many modern oscilloscopes, or by capturing a time trace at
                        high speed and performing the spectral analysis off line in a computer. Careful
                        measurement throughout, for example of the audio frequency band, will often
                        point out many areas that are best avoided.


            5.5 Building the Synchronous Detector
                        At low frequencies (<1MHz), a wide variety of analog operational circuitry can
                        be used to construct the four-quadrant multipliers necessary to multiply two
                        sine waves. It is easiest to use ICs such as the Analog Devices AD534/634 or
                        Burr-Brown MPY100. However, they are complex and typically provide only


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