Page 187 - Photodetection and Measurement - Maximizing Performance in Optical Systems
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Stability and Tempco Issues

            180   Chapter Eight


                                                        Clamped
                                                        fiber


                                             Steel
                                  Plastic    mandrel
                                  supports


                                                                   Monitor
                                                                   photodiode
                                  Glass
                                  waveguide    N
                                                   Magnet

                        Figure 8.15 Light can be tapped from a fiber using a small-radius bend.
                        A magnet and steel mandrel make a convenient clamp, and even allow
                        the light to be coupled to an embedded photodiode.


                        fiber with a known radius of curvature and to press it against a glass baseplate.
                        If a primary-coated fiber is used, light couples out of the coating and into the
                        glass slide at the point of contact. The glass plate acts as a simple light-guide
                        coupling to a small photodiode such as a BPW34. The steel mandrel can be held
                        in place using a small magnet fixed underneath the glass.
                          Schemes for optical referencing in these ways provide some of the highest
                        resolution measurement techniques available. The papers by Allen (1995) and
                        Imasaka (1983) give good examples of what is possible in chemical photometry.

            8.5.3 Intensity noise reduction
                        Dual-detector referencing has another very important use—source noise reduc-
                        tion. In systems that have high received optical powers, which should easily be
                        shot-noise limited in detection, the measured noise level is often found to be far
                        greater than expected from the shot calculation. This is because the source itself
                        exhibits excess intensity noise. Sometimes this is due to poor regulation of
                        the power supplies feeding the source. This can usually be seen with a low-
                        frequency spectrum analyzer. Even with good supplies, laser systems in partic-
                        ular are prone to excess noise, usually exacerbated by spurious optical feedback
                        into the laser cavity from lenses, windows, fibers etc. Even focussing the laser
                        beam with a microscope objective onto a cleaved fiber end-face for coupling
                        forms an efficient retroreflector. The noise level is often 30 to 60dB worse than
                        shot noise. Just as we can suppress slow intensity drifts caused by source
                        temperature fluctuations, so we can use the configurations such as seen in
                        Fig. 8.10 to reduce the effects of fast excess intensity noise. For example, we
                        can divide signal by reference in an analog divider IC as previously mentioned
                        (Fig. 8.16a). Alternatively, if the two signals are adjusted to be nominally equal,
                        they can be subtracted to achieve the same compensation (Fig. 8.16b). This is
                        capable of lower noise and higher bandwidth.

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