SEMICONDUCTOR DEVICE PHYSICS AND DESIGN

(Greg DeLong) #1
112 CHAPTER 3. CHARGE TRANSPORT IN MATERIALS

102
ELECTRIC FIELD (V/cm)

CARRIER

DRIFT

VELOCITY

(cm/s)

103 104 105 106

105

106

107

108

GaAs

Si

InP

Electrons
Holes

Figure 3.10: Velocity–field relations for several semiconductors at 300 K.

The corresponding relaxation times are

τsc(1 kV/cm) =

(0. 26 × 0. 91 × 10 −^30 kg)(1400× 10 −^4 m^2 /V)
1. 6 × 10 −^19 C

=2. 1 × 10 −^13 s

τsc(100 kV/cm) =

(0. 26 × 0. 91 × 10 −^30 )(100× 10 −^4 )

1. 6 × 10 −^19

=1. 48 × 10 −^14 s

Thus the scattering rate has dramatically increased at the higher field.

Example 3.8The average electric field in a particular 0.1μm GaAs device is 50 kV/cm.
Calculate the transit time of an electron through the device (a) if the transport is ballistic;
(b) if the saturation velocity value of 10^7 cm/s is used.
For ballistic transport the transit time is

τtr=


2 L

a

with the acceleration,agiven by
a=

eE
m∗
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