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An Intr oduction to Or ganic Photodetectors     259






                          Noise-free
                   R
                           resistor
                                                                  Z
                                                                   C
                                        C            σ VC (f ) = σ ∼ V Δf  R + Z C
                     σ ∼    Voltage
                      V
                          noisesource



               FIGURE 6.36  A noisy resistor can be represented by a noise-free resistor in
               series with a noisy voltage source. The noise due to the resistor can be
               determined by considering the behavior of an RC circuit.


               the capacitor and resistor as a potential divider, the corresponding
               voltage σ  across the capacitor is given by
                       VC


             σ   () f =     f Δ  Z C  =     f Δ  1 /(2 πjfC )  = σ  f Δ  1
                                    σ
                     σ
               VC     V     R +  Z   V     R + 1 /(2 πjfC) )  V  12
                                                                + πjfCR
                                C
                             f Δ
                        σ
                   =     V
                      1  + 2   ) 2
                         ( πfCR
               Hence, squaring and integrating over all frequencies, we obtain for
               the total noise variance
                                         2
                                    ∞   σ df      σ 2
                                  =
                              σ VC ∫     V    2  =  V
                               2
                                    0  1 + ( 2 πfCR)  4CR
               Rearranging, we obtain

                                2
                               σ =  8 R ⎛ ⎜  1  C σ 2  ⎞ ⎟  =  8 R U
                                V     ⎝ 2  VC ⎠

               where 〈U〉 can be identified as the time-averaged energy stored by the
               capacitor.  From the equipartition theory of classical thermodynam-
                       51

               ics, 〈U〉  is equal to 1/2k T. Hence, we obtain for  σ  2
                  51
                                    B                      V

                                    σ  2  =  4 kTR
                                      V    B
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