Page 42 - Photodetection and Measurement - Maximizing Performance in Optical Systems
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Amplified Detection Circuitry

                                                                    Amplified Detection Circuitry  35

           2.7.2 TRY IT! Resistor choice
                         Once again, make a transimpedance amplifier based on an FET opamp. Perhaps you
                         should chose the fastest amplifier from the previous TRY IT!. This time let’s really go
                         for speed and choose the lowest capacitance photodiode available. Borrow a selection
                                                      2
                         of 100-MW resistors. I used a 1-mm UDT PIN040A photodiode with 15-V reverse bias,
                         an OPA604 opamp, and six different 100-MW resistors. These range from a 50-mm-
                         long plate construction device used for 500-VAC operation to a standard axial leaded
                         0.25W device and a couple of 1 ¥ 2-mm chip resistors.
                           Illuminate the photodiode with a red LED connected to a square-wave generator,
                         but keep it far enough away not to couple it electrically. This is often visible as greatly
                         enhanced flanks on the received square wave. This is a spurious coupling via the capac-
                         itance between LED leads and photodiode leads and gives a high-pass characteristic
                         coupling response. A 100-mm glass or grounded metal tube with an LED and photo-
                         diode lodged in each end can be used to increase optical coupling efficiency. Alterna-
                         tively, a fiber could be used, albeit with a lot more work.
                           Connect the resistors one at a time and observe the transition rise times. I oper-
                         ated at 5kHz and used a socketed FET opamp with pins 2 and 6 bent up out of the
                         socket for flying connections. My results are shown in Fig. 2.13a. First we can see the
                         gross differences in performance. The plate resistors show several cycles of overshoot,
                         which can be attributed to the distributed capacitance of these large devices. However
                         even the “normal” components show big differences, with 10 to 90 percent rise time





                          10
                                       Large plate
                           8
                                         Medium plate
                              Chip
                           6

                           4
                         Intensity  2  1/4W axial



                           0

                          -2


                          -4
                          -6
                           -250   -200  -150   -100   -50    0     50    100    150   200    250
                                                          Time (ms)
                       Figure 2.13a Response of a transimpedance amplifier for a selection of 100-MW resistor types,
                       including large plate types, 1/4-W axials and a chip types. The fastest response was obtained with
                       a chip component.


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