Page 33 - Photodetection and Measurement - Maximizing Performance in Optical Systems
P. 33

Amplified Detection Circuitry

            26   Chapter Two

                        coupling to optical fibers. (see Table 1.2 for a few examples.) When speed is the
                        key parameter, and all the light can be collected by the diode, the smallest pos-
                        sible device should be selected. For example, in a typical single-mode fiber com-
                        munications receiver, infrared light is guided in a fiber core with a mode
                        diameter of the order of 10mm. If the coupling tolerances can be handled and
                        the fiber can be positioned close enough to the chip, this is as large as the pho-
                        todiode needs to be (Fig. 2.5a). Photodiodes are available with a diameter of
                        25mm; this is small, but the area is still approximately 10 times bigger than
                        necessary. Although at these small sizes the capacitance is unlikely to reduce
                        proportionately to area, some gain in improvement is inevitable with smaller
                        devices.


            2.4.3 Optical transforms
                        We could in principle do even better with optical matching of source and detec-
                        tor. Liouville’s theorem states that the étendue of an incoherent optical system
                        cannot be reduced, but it can at least be manipulated. The étendue can here be
                        thought of as the product of the beam’s area and the square of the numerical
                                    2
                        aperture (NA ). The light’s NA on exiting the fiber is only about 0.12 and the
                                                2
                                                                          2
                        mode area is about 100mm , giving a product of 1.4mm . Now, unless restricted
                        by packaging, the photodiode can accept light over its full area and almost 2p
                                               2
                        steradians, about 0.5NA . Hence if we can fill this acceptance NA, it can be
                        traded for a reduction in spot size. We can use a microoptic lens system to do
                        this (Fig. 2.5b), forming a spot of approximately 1.6mm diameter. This is as big
                        as the photodetector needs to be. The capacitance of such a small detector could
                        be far less than that of conventional, even very small devices. If this could be
                        used without being swamped by transistor and packaging capacitance, power
                        lost in high-angle Fresnel reflection coefficients or in positioning tolerances,
                        performance improvements would be expected. It would be most convenient if
                        the microoptic lens were integrated permanently with the tiny photodiode, for
                        illumination from the single-mode fiber or fused onto the fiber end. At least
                        one company (ALPS Electric) offers lenses and lensed detectors with this



                        (a)                   (b)






                            2
                                                                   2
                                               2
                         NA =0.014           NA =0.014           NA =0.5
                         Area 100mm 2        Area 100mm 2        Area 2.8mm 2
                        Figure 2.5 Careful alignment of single-mode optical fibers allows the
                        use of photodiodes with very small areas (<30mm diameter). Increas-
                        ing the numerical aperture (NA) of the incident light in principle
                        allows the use of even smaller detectors.

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