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System Noise and Synchronous Detection

                                                         System Noise and Synchronous Detection  113


                                                       Multiplier  RC time
                                        Two-channel            constant
                                        lock-in amplifier              Voltage
                                                                       display
                                                                       P cos j

                                       Scope                 Ref. input (cos)
                                                               +90°

                                        Noisy signal   Signal   Multiplier  RC time
                                                       inputs           constant
                                                                                Voltage
                       Generator                                                display
                       crystal controlled                                       P Sin j
                       7.200kHz
                                                                     Ref. input (sin)



                                                      -
                                                                         Generator
                                                      +
                                                   Transimpedance        crystal controlled
                                                   receiver              7.195–7.205kHz
                       Figure 5.22 The lock-in reference signal need not come from the source modulator. As
                       long as the frequency difference is small enough to remain within the filter bandwidth,
                       separate oscillators can be used. However, two-phase detection will be needed to measure
                       the signal amplitude independent of drifting phase.


                       will be correctly detected, although a single-channel lock-in will show periodic
                       positive and negative output excursions as the phase varies. Taking the square
                       root of the sum of the squared outputs from a two-channel lock-in, driven by
                       sine and cosine references, we obtain a stable determination of the magnitude
                       of the detected signal, without signal fading due to the slow phase variations.
                       The two-channel lock-in provides the sum-of-squares computation via its
                       magnitude/phase setting (sometimes labelled “Rq”). Let’s look at a nonsyn-
                       chronous experiment in some more detail.


           5.7.5TRY IT! Non-phase-synchronous signals
                         The lock-in lends itself supremely to experimentation. There is sufficient complexity
                         to test many different aspects of signal processing, but it has sufficient precision to
                         make it all convincingly close to theory. Set up two oscillators, one being preferably
                         crystal controlled and the other variable. The crystal oscillator could be made
                         with 32kHz watch crystals and two divided by two flip-flops (see Fig. 6.8). I had a
                         3.6864MHz crystal divided down to about 7.2kHz using an HC4060 chip. Use this to
                         drive the reference input of your lock-in amplifier.
                           The other oscillator should be tunable around the reference frequency and as stable
                         as possible. If you have a nice synthesized source, settable to a fraction of a hertz, all
                         the better, but this TRY IT! can be done even with a dial-tuned analog oscillator with
                         a little care. To be proper about this, you could drive an LED from the oscillator and


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