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Amplified Detection Circuitry

                                                                    Amplified Detection Circuitry  31

                       quency values. While 15.8k from the E96 series and precision capacitors will
                       reduce the error such effort is probably wasted on this application.
                         When building transimpedance amplifiers with high value resistors, say,
                       10MW and up, often no parallel capacitance is needed, not even a few mil-
                       limeters of twisted wire-wrap wire. Even without it the circuit is overdamped.
                       This may be because the capacitance of the resistor itself is sufficient. Axial
                       geometry 0.4-W metal-film resistors typically show a terminal capacitance of
                       the order of 0.1 to 0.2pF. This means that with a 100-MW resistor, the imped-
                       ance of the combination will drop above about 8 to 15kHz due to this effect
                       alone. Add to this variables such as circuit strays and PCB tracks, and it will
                       be a struggle to get even this bandwidth. This is discussed in more detail later
                       in this chapter.
                         As we have seen, the transimpedance amplifier can be used with a completely
                       unbiased detector and still give a linear response. Without deliberate bias, the
                       voltage across the photodiode is just the offset voltage of the amplifier. We will
                       assume that this is zero, although even a few millivolts here can significantly
                       affect noise performance, especially if the photodiode has a low shunt
                       resistance.



           2.6 Increasing Bandwidth with Loop-Gain
           2.6.1 Opamp choice
                       We have seen that one key to overall photoreceiver detection speed is “gain
                       bandwidth” of the amplifier used in the transimpedance configuration. In
                       an earlier section the bandwidth of a 720-pF/1-GW receiver was increased from
                       0.22Hz to 363Hz through the use of a 0.6-MHz GBW opamp, the improvement
                       going approximately as the square root of GBW. Many other devices with higher
                       gain bandwidths are available. For example many common junction FET
                       (JFET) opamp families such as LF353, LF412, TL081, OPA121, AD711 have
                       GBWs around 4MHz. The OPA604 offers 20MHz. This should increase our
                       example system’s bandwidth to 2kHz. A few specialist FET amplifiers are avail-
                       able with even greater GBWs. The Burr-Brown (now part of Texas Instruments)
                       OPA657 JFET opamp has GBW = 1.6GHz, and a unity gain stable device has
                       230MHz. In theory this would push our detection bandwidth to 7kHz.


           2.6.2 TRY IT! Opamp choice
                         Set up a 100-MW transimpedance receiver with a small photodiode with about
                         100-pF capacitance. If this is not available, use a small photodiode with a 100-pF
                         capacitance across it. In a voltage follower configuration we would obtain a detection
                         bandwidth on the order of 16Hz, or a transient rise time of about 0.35/16 = 22ms.
                         Use an integrated circuit socket for the opamp. Now take a selection of opamps and
                         observe the variation of transient response for a 5-kHz square-wave input. Figure 2.9
                         shows my results with a few opamps from the collection. It is clear that the majority
                         of devices from this collection perform similarly, with rise times of 20 to 50ms, whereas


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