Title: OUTLINE
1Lecture 28
- OUTLINE
- The BJT (contd)
- Small-signal model
- Cutoff frequency
- Transient (switching) response
- Reading Pierret 12 Hu 8.8-8.9
2Small-Signal Model
Common-emitter configuration, forward-active mode
R. F. Pierret, Semiconductor Device Fundamentals,
Fig.12.1(a)
hybrid pi BJT small signal model
Transconductance
EE130/230A Fall 2013
Lecture 28, Slide 2
3Small-Signal Model (cont.)
where QF is the magnitude of minority-carrier
charge stored in the base and emitter regions
forward transit time
EE130/230A Fall 2013
Lecture 28, Slide 3
4 Example
A BJT is biased at IC 1 mA and VCE 3V. bdc
90, tF 5ps, T 300K. Find (a) gm , (b) rp ,
(c) Cp .Solution (a) (b) rp bdc /
gm 90/0.039 2.3 kW (c)
EE130/230A Fall 2013
Lecture 28, Slide 4
5Cutoff Frequency, fT
The cutoff frequency is defined to be the
frequency (f w/2p) at which the short-circuit
a.c. current gain equals 1
EE130/230A Fall 2013
Lecture 28, Slide 5
6For the full BJT equivalent circuit
fT is commonly used as a metric for the speed
of a BJT.
Si/SiGe HBT by IBM
- To maximize fT
- increase IC
- minimize CJ,BE, CJ,BC
- minimize re, rc
- minimize tF
EE130/230A Fall 2013
Lecture 28, Slide 6
7Base Widening at High IC Kirk Effect
For a NPN BJT
- At very high current densities (gt0.5mA/mm2), the
density of mobile charge passing through the
collector depletion region exceeds the ionized
dopant charge density
increasing IC
- ? The base width (W) is effectively increased
(referred to as base push out) - ? tF increases and hence fT decreases.
- This effect can be avoided by increasing NC ?
increased CJ,BC , decreased VCE0
EE130/230A Fall 2013
Lecture 28, Slide 7
C. C. Hu, Modern Semiconductor Devices for
Integrated Circuits, Figure 8-18
8Summary BJT Small Signal Model
Hybrid pi model for the common-emitter
configuration, forward-active mode
EE130/230A Fall 2013
Lecture 28, Slide 8
9BJT Switching - Qualitative
R. F. Pierret, Semiconductor Device Fundamentals,
Figs. 12.3-12.4
EE130/230A Fall 2013
Lecture 28, Slide 9
10Turn-on Transient Response
- The general solution is
- Initial condition QB(0)0 since transistor is
in cutoff
where IBBVS/RS
EE130/230A Fall 2013
Lecture 28, Slide 10
R. F. Pierret, Semiconductor Device Fundamentals,
Fig. 12.5
11Turn-off Transient Response
- The general solution is
- Initial condition QB(0)IBBtB
EE130/230A Fall 2013
Lecture 28, Slide 11
R. F. Pierret, Semiconductor Device Fundamentals,
Fig. 12.5
12Reducing tB for Faster Turn-Off
- The speed at which a BJT is turned off is
dependent on the amount of excess
minority-carrier charge stored in the base, QB,
and also the recombination lifetime, tB. - By reducing tB, the carrier removal rate is
increased - Example Add recombination centers (Au atoms) in
the base
EE130/230A Fall 2013
Lecture 28, Slide 12
13Schottky-Clamped BJT
- When the BJT enters the saturation mode, the
Schottky diode begins to conduct and clamps the
C-B junction voltage at a relatively low positive
value. - ? reduced stored charge in quasi-neutral base
EE130/230A Fall 2013
Lecture 28, Slide 13
R. F. Pierret, Semiconductor Device Fundamentals,
Fig. 12.7