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Photodiodes

                                                            Photodiodes  47

          a photodiode. In fact, light-emitting diodes behave like photodiodes un-
          der illumination. In the inset, we show the diode I–V as captured on a
          curve tracer. The graph shows the measurement of the forward char-
          acteristic on a semilog scale. There is a region near zero bias where the
          log of the current is proportional to the bias voltage. The slope of the
          curve in this region is used to calculate n. In this case, n = 1.38.
            The photocurrent is given accurately by Eq. 3.14, and you should be
          able to verify the linear dependence of the photocurrent on the inci-
          dent light intensity over several orders of magnitude of incident light
          intensity.


          3.3  Photodiode Operation: The Photocurrent Mode
          and the Photovoltage Mode

          Photodiodes can be operated in two modes: as a source of photocur-
          rent or as a source of photovoltage. In the photocurrent mode, the
          photodiode is given a reverse bias that is large enough to put the
          diode in the voltage-independent dark current regime. In Fig. 3.4 you
          can see that 0.5 volts would be sufficient. The dependence of photocur-
          rent on photon flux has already been given in Eq. 3.15.
            In the photovoltaic mode, the output of the diode is measured with
          a high-impedance voltmeter so that the photocurrent is near 0. This
          mode of operation has the advantage that it is about the simplest way
          to derive a signal from a photodiode. It requires, in principle, no other
          circuit elements. In some real applications, this may be all that is
          needed. Setting the current = 0 in Eq. 3.14,
                                         2
                                     qD e n i  qV A /kT
                             qG L L e =    (e     – 1)
                                     L e N A
                                               2
                                        N A G L L e
                                qV A /kT
                               e      =         + 1                  (3.17)
                                             2
                                          D e n i
          where V A is the photovoltage generated by the photodiode. Solve for
          V A by taking the natural log of both sides:
                                  kT       N A G L L e 2
                             V A =    ln         + 1                 (3.18)
                                   q       D e n i 2
          This equation shows that the photovoltage is not a linear function of
          photon flux. There are some important practical implications of this
          result. When used in the photovoltage mode:

          a. The photovoltage response is nonlinear.
          b. The response is not easy to model for correction.



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