Page 263 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
P. 263

RADIATION  SENSORS    243

                  UV        Vis   Near IR        Thermal IR
              Wavelength (Um)
                    I          1  I  T                  i  r     1
                   0.2    0.4  0.6  0.8  1              8  10    20
                           Si





                                    Ge
                                        PbS
                                          PbSe
                                      InAs (77 K)
                                           InSb(77K)
                                                MCT (77 K)
                                          Pyroelectric detectors


   Figure  8.15  Some  common  semiconducting materials  used  in  radiation  microsensors  and  their
   dynamic range  within  the UV-to-IR spectrum
   The  most  obvious advantage  of a photovoltaic  cell  over a photoconductive cell  is that it
   is  compatible  with  a  bipolar  process  (e.g.  Si  or  GaAs).  However,  the  reduced  size  and
   integrated  electronics lead  to a higher  sensitivity,  faster response  time  (us instead  of ms),
   and better stability.
     Photosensitive diodes, known as photodiodes,  can be made in a standard vertical bipolar
   process  (see  Section  4.3.4)  such  as  a  p-n  diode,  or  variations  on  this  process,  such  as
   a  /7-Si/insulator/n-Si PIN  diode,  Schottky-type  diode,  and  silicon  avalanche  diode  (see
   Figure  8.16).
     The basic  principle  of all  these  photodiodes  is that the photon creates  an  electron-hole
   pair  in  the  space-charge  region  of  the junction.  These  charges  are  then  separated  by  the
   local field to the different  doped regions, and they modify  the diode voltage  V d. The diode
   voltage  is the  open  circuit voltage  V oc and can  be measured by reverse-biasing  the  diode
   and finding the  voltage  dropped  across  a high  external  load  resistor  R L.  Then  the output
   voltage  is given  by


                              In     —  I  and  so  V oc a  In(I R)     (8.19)

   where  I R  is  the  photocurrent  and  is  proportional  to  the  intensity  of  incident  radiation
  and,  as  usual,  I s  is  the  reverse  saturation  current.  Indeed,  this  equation  is  the  same  one
  that  applied  to  a  thermodiode  (see  Section  8.2.1  and  Equation (8.9)),  and  so  the  device
  will  normally  be  temperature-sensitive.  Thus,  the  performance  of  a  photodiode  can  be
  improved by either running it at a constant  voltage  -  as low as possible to reduce junction
  noise -  or it must be temperature-compensated.
     An  alternative  approach  is  to  fabricate  a  phototransistor  rather  than  a  diode.  Like
  a  PTAT device,  an  IC  can  be  built  using  two  identical  transistors;  the  first  produces  a
  photoinduced collector  current I CR and the other produces a reference collector current I C0.
   258   259   260   261   262   263   264   265   266   267   268