Page 295 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
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MAGNETIC  SENSORS     275
























                           10 1
                              0       0.5    1.0     1.5
                                 Magnetic  flux  density, B(T)

  Figure  8.41  Response of a InSb/InSb magnetoresistive device to an applied magnetic flux density

  8.5.3  Magnetodiodes and Magnetotransistors

  Figure  8.42  shows  the  schematic  layout of  two types of diode.  The  first  is  made using a
                                                                        +
  silicon-on-sapphire  (SOS) IC process  in which carriers  are injected from  both  the n  and
   +
  p  junctions and  drift  under the  action  of the  electric  field.  The  magnetic flux density is
  applied  perpendicular  to  the  carrier  flow,  and  a  difference  in  the  recombination  rates  at
  the two junctions occurs  (Suhl effect).  The  difference  in recombination rates modifies the
  I-V  characteristics  of the  diode,  and the  forward voltage  sensitivity  is given  by,


                            dV f
                         =                            •v;              (8.46)
                      S v
                            dB
  where  ^ n  and  IJL P  are the  electron  and  hole  mobilities,  r eff  is the effective  lifetime  of the
  carrier,  v\  and  v 2  are  the  recombination  rates  at  the  two junctions,  and  the  thickness d
         –
  of the  n  diffusion  region  is  less  than the  ambipolar  diffusion  length. The  SOS structure
  provides  high  recombination  on  one  side  (Si—Al 2O 3)  and  low  on  the  other  (Si—SiO 2)  to
  give  a  sensitivity  S v  of  about 5 V/T  (Lutes et al.  1980).  However,  this  device  is highly
  nonlinear  and  has  an  output  that  depends  strongly  on  temperature  or  the  roughness  of
  the  two  surfaces.  The  second  structure  can  be  made  from  a  standard  IC  process,  for
  example,  CMOS.  The  device  looks  like  a  transistor  but  is  operated  as  a  diode,  and  the
  reversed  biased  p-n  (collector) junction becomes  the high recombination  surface. When
  the  magnetic  field  is  applied,  the  collector  current  I C  changes  and  so  does  the  base
  resistivity  and  hence  the  base-emitter  voltage  V BE  This  can  produce  a  forward voltage
  sensitivity  of  about  25 V/T  (Popovic  et al.  1984)  that  is  five  times  greater  than  that  of
  the  SOS device.
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