Before we leave diodes, it would be worthwhile exploring some
other modes of operation, as well as some specific applications
which will be of interest. We said that when the diode was
reverse-biased (p-region negative with respect to the n-region)
that the only current which flows is the reverse saturation
current, resulting from the few thermally generated minority
carriers which can fall down (or up) the barrier (Figure 1).
If we make the reverse bias even greater, the same current
flows, but the carriers pick up more energy as they fall down
the (now larger) junction potential. As they do this, it is
possible for them to pick up so much energy, that when they
collide with a lattice site, they create an additional
electron-hole pair through a process called
impact
ionization (
Figure 2). When this occurs,
we now have current consisting of two electrons and one
hole. These additional carriers can themselves collide and
generate additional electron hole pairs as well. The current now
consists of five electrons and two holes. This process is called
avalanche multiplication (
Figure 3), because we start with one carrier, and
through a succession of impacts create more and more
current. This process can in fact run away, much like an
avalanche on a snowy mountain side, in a process called
avalanche breakdown.
The net effect is to change the reverse characteristics of the
diode somewhat. If we include the effect of breakdown in the I-V
curve for the diode, we would see something like that in
Figure 4.
There is now a sudden onset of current after the avalanche
breakdown voltage has been exceeded. Do not be confused into
thinking that this "breakdown" means that the diode has been
damaged. The process of avalanching itself is not
destructive. But as you can see from Figure 2,
the diode current increases very rapidly once the breakdown
threshold has been exceeded. Thus, if there is not something in
series with the diode to limit the maximum current through it,
it could be damaged by overheating. Diodes in breakdown are used
as voltage references (the voltage across them is more or less
independent of the current running through them) but you will
always find a series current limiting resistor used along with
them. Such diodes are called Zener Diodes (named
after the grandfather of Will Rice's George Zener who graduated
a few years ago...that is George did, not his grandfather) but
the name is kind of a misnomer. The Zener Effect is
also a reverse breakdown phenomena, but comes from direct field
generation of extra carriers, rather than as a result of impact
ionization. In truth, you can not tell the one effect from the
other by looking at the diode I-V curve, and so all diodes used
in reverse breakdown are called Zener Diodes. A circuit using a
Zener diode as a voltage reference is shown in Figure 5.
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