376 SEMICONDUCTOR DEVICES
Figure 7.4.9p-channel enhancement MOSFET.(a)Cross-sectional structure.(b)Symbol.
MOSFETs, like JFETs, arenormally ontransistors, in which the field effect reduces conduction
by depleting the built-in channel. Figure 7.4.11(a) shows the formation of depletion regions due
to electron-hole recombinations with a negative gate voltage. WithvGS≤−VP, whereVPis the
pinch-off voltage, the depletion regions completely block the channel, makingiD=0, as shown in
Figure 7.4.11(b), which corresponds to the cutoff condition. WithvGS>−VPandvGD<−VP,
so thatvDS>vGS+VP, the channel becomes partially blocked or pinched down when the device
operates in its active state.
Figure 7.4.12 shows the characteristics of a typicaln-channel depletion MOSFET. With
VP =3V,iD=0 forvGS≤−3V.If−3V<vGS≤0, the device operates in the depletion
mode; ifvGS>0, it operates in the enhancement mode. The equations describing the drain current
are of the same form as for the JFET.
In the ohmic region, whenvDS<vGS+VP,
iD=IDSS
[
2
(
1 +
vGS
VP
)(
vDS
VP
)
−
(
vDS
VP
) 2 ]
(7.4.11)
In the active region, whenvDS≥vGS+VP,
D (drain)
S (source)
D
S
+
+
− −
(gate) G
G
vGS
vDS
iD
Heavily
doped
Oxide
layer
Metallic
film
(a) (b)
D
S
−
−
+ +
G
vSG
vSD
iD
(c)
n–channel
n p
n+
n+
Figure 7.4.10Depletion MOSFETs.(a)Structure ofn-channel depletion MOSFET.(b)Symbol ofn-channel
depletion MOSFET.(c)Symbol ofp-channel depletion MOSFET.