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Electrical Response Time of Diodes

                                           Electrical Response Time of Diodes  67

          where W, the width of the region separating the charge, is easily cal-
          culated by using Poisson’s equation:
                                 2   0    N A + N D      1/2
                          W =                 (V Bi – V)               (4.6)
                                 q
                                      N A N D
            The relative dielectric constant of common semiconductors is in the
          range of 10–13, and A is the area of the diode. The capacitance is ob-
          tained by substitution of Eq. 4.5 into Eq. 4.4. In nearly all diodes, the
          concentration of donors, N D is orders of magnitude different from the
          concentration of acceptors,  N A . For example, if  N A is 10 19  cm , N D
                                                                     –3
                                  –3
          might typically be 10 16  cm . Assuming that N A   N D , we can simplify
          the expression for the capacitance further:
                                    A
                                                        0 qN D
                                   q  N             2(V Bi – V)

                     C =    0       (V Bi – V)  = A                    (4.7)
                               2   0
                                         D
            In Eqs. 4.6 and 4.7, V Bi is the built-in voltage of the diode and N D is
          the impurity concentration on the less heavily doped side of the junc-
          tion.
            This relationship shows that the capacitance will be larger if the im-
          purity concentration on the less heavily doped side of the junction, N D ,
          is increased. Since N D is fixed at the moment of fabrication, there is
          nothing you can do about this parameter except to measure it and look
          for a photodiode from another source with a lower value for N D . The ca-
          pacitance also depends directly on the area. That is: size matters. The
          capacitance varies inversely with the square root of the bias voltage,
          and you can lower the capacitance significantly by increasing the bias
          voltage. The reduction of capacitance leads to a corresponding reduc-
          tion in the extrinsic response time. Furthermore, this is the only post-
          fabrication means of changing the response time of a photodiode.


          Example 4.2
          Find the capacitance of a silicon photodiode at 0 bias. The diode is a
          square chip 1 mm × 1 mm and has a doping concentration of 1 × 10 16
             –3
          cm .

                                         0 qN D
                             C = A            (farads)
                                    2(V Bi – V)
          C =

                                         –14
                                                                   16
                                                          –19
                                                                        –3
                                           (F/cm) · 1.6 × 10
                                                            (C)·10 (cm )
                            9.5 · 8.85 × 10
                        2
            (0.1 × 0.1)(cm )
                                             2(0.8 – 0) volts
                                 C = 289 picofarads
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