Figure 10.30Operation of a semi-
conductor diode.
(a) When there is no applied
voltage, the thermal electron
current to the right equals the
recombination electron cur-
rent to the left and there is no
net current. Both these cur-
rents are small.
(b) When an external voltage is
applied so that the pend of
the diode is negative, the re-
combination electron current
is less than the thermal elec-
tron current. The result is a
very small net electron cur-
rent to the right.
(c) When an external voltage is
applied so that the pend of
the diode is positive, the re-
combination current can be
much larger than the thermal
electron current to give a large
net electron current to the left.
The conventional current is in
the opposite direction to the
electron current.
free electron
hole
= thermal electron current
= recombination electron current
it
ir
New
holes
created
V
+
it
New
electrons
ir added
Electrons and holes
recombine at junction
eF(n)
eF(p) Ve
(c) Forward bias
(a) No bias
it
ir
p region n region
p-n junction
Electron
energy
Depletion region Valence band
Forbidden
band
iirtConduction band
eF
(b) Reverse bias
Holes
disappear
+
V
it
ir
Electrons
disappear
eF(n)
eF(p) Ve
Figure 10.31Voltage-current characteristic of a p-nsemiconductor diode.
Reverse bias Forward bias
V
I
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