Page 94 - Photodetection and Measurement - Maximizing Performance in Optical Systems
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Interlude: Alternative Circuits and Detection Techniques

                                               Interlude: Alternative Circuits and Detection Techniques  87

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                         Voltage (mV)  20




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                                             8 fine black stripes             2 broad
                                                                              black stripes
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                           -2500        -1500        -500         500          1500         2500
                                                          Time (μs)
                       Figure 4.7 Self-detecting LED output for eight 1-mm-wide black stripes on a retroreflecting disk.


                       trum. Emission wavelengths are usually in the 610 to 640nm range. In princi-
                       ple they could be coupled with a silicon detector to give improved sensitivity
                       beyond 1mm wavelength, but in practice it is far better to use a germanium or
                       InGaAs photodiode.
                         Below 350nm most silicon detectors also show poor and decreasing respon-
                       sivity, due both to use of a borosilicate glass or plastic window and to the intrin-
                       sic detection process. Especially at these ultraviolet wavelengths, therefore,
                       fluorescent wavelength conversion is an attractive option. The goal is to find a
                       material with high absorption at the “difficult” wavelength, which reemits in a
                       longer-wavelength region where the photodiode sensitivity is superior (Fig. 4.8a
                       and b). If the emission process is efficient, there can be a net gain in detection
                       sensitivity. A number of fluorescent glasses, polymers, and dyes is available for
                       this. For example, Sumita Optical Glass manufactures a range of fluorescent
                       glasses that can be mounted directly on the front of the photodetector as a wave-
                       length converter. Some can also be processed into planar waveguide form with
                       edge-mounted detectors, allowing large areas for detection of diffuse or widely
                                                               2
                       dispersed light (Fig. 4.8c). Large-core (mm ) optical fibers can be formed from
                       some fluorescent polymers. The best materials for this use show high absorp-
                       tion at the detected wavelength and low absorption at the shifted wavelength,
                       so that self-absorption of the visible light is minimized. With the great interest
                       in and potential markets for efficient white-light LEDs, it is likely that big
                       improvements will be seen in phosphor materials for use at deep blue/near-UV


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