256 CHAPTER 6. BIPOLAR JUNCTION TRANSISTORS
pe(xe = 0) nb(x)Emitter VBE Base VCB Collectorpeopbo ncopcoIE
|EBJ| | CBJ |
depletion
layerdepletion
layer (a)nboEquilibrium densityWbnneo– + –+
xe xc(b)p nbo
eoxe = 0xb= 0
xb =Wbn x
c = 0xbpcoWbIB IC
Forward bias Reverse biasFigure 6.7: A forward active mode BJT. (a) The equilibrium carrier concentrations of electrons
and holes and positions of the junction depletion regions in thenpntransistor. (b) Minority
carrier distributions in the emitter, base, and collector regions.
The profile of the total minority carrier densities (i.e., background and excess) is shown in fig-
ure 6.7b. The electron distribution in the base is almost linear, as can be seen, and is assumed
to be so for some simple applications. Once the excess carrier spatial distributions are known
we can calculate the currents as we did for thep-ndiode. We assume that the emitter-base cur-
rents are due to carrier diffusion once the device is biased. We have, for a device of areaAand