SEMICONDUCTOR DEVICE PHYSICS AND DESIGN

(Greg DeLong) #1
332 CHAPTER 7. TEMPORAL RESPONSE OF DIODES AND BIPOLAR TRANSISTORS

Example 7.1Consider annpntransistor with the following properties at 300 K:

Emitter current, IE =1.5mA
EBJ capacitance, Cje =2pF
Base width, Wb =0. 4 μm
Diffusion coefficient, Db =60cm^2 /s
Width of collector depletion region, Wdc =2. 0 μm
Collector resistance, rC = 30Ω
Total collector capacitance, (Cs+Cμ)=0. 4 pF
Saturated electron velocity, vs =5× 106 cm/s

Calculate the cutoff frequency of this transistor. How will the cutoff frequency change (i)
if the emitter current level is doubled? (ii) if the base thickness is halved?
The emitter resistancer


eis given by (see equation 7.5.11 for the resistance of a
forward-biased diode)

r


e=

dIE
dVBE

∼=kBT
eIE

=

0. 026

1. 5 × 10 −^3

=17.3Ω

This gives
τe=r


eCje=(17.3)(2×^10

− (^12) )=34.6ps
The base transit time is
τt=
Wb^2
2 Db


=

(0. 4 × 10 −^4 )^2

2 × 60

=13.3ps

The collector transit time is

τC=

Wdc
2 vs

=

(2. 0 × 10 −^4 )

1 × 107

=10ps

The collector charging time is

τc=rc(Cμ+Cs) = 30(0. 4 × 10 −^12 )=12ps

The total time is
τec=34.6+13.3 + 10 + 12 = 69.9ps
The cutoff frequency is

fτ=

1

2 πτec

=

1

2 π(69. 9 × 10 −^12 s)

=2.3GHz

If the emitter current is doubled (assuming no other change occurs), the timeτeis reduced
by half. This gives a cutoff frequency of 2.54 GHz. Similarly, if the base width is reduced
by half, the base transit time becomes 3.3 ps and the cutoff frequency becomes 2.65 GHz.
In this problem the dominant source of delay is the emitter junction.
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