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Heterojunction%20Bipolar%20Transistors

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Heterojunction Bipolar Transistors for High-Frequency Operation D.L. Pulfrey Department of Electrical and Computer Engineering University of British Columbia – PowerPoint PPT presentation

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Title: Heterojunction%20Bipolar%20Transistors


1
Heterojunction Bipolar Transistors for High-Frequ
ency Operation
Day 3A, May 29, 2008, Pisa
2
Outline
  • What are the important features of HBTs?
  • What are the useful attributes of HBTs?
  • What are the determining factors for IC and IB?
  • Why are HBTs suited to high-frequency operation?
  • How are the capacitances reduced?

3
Schematic of InGaP/GaAs HBT
  • Epitaxial structure
  • Dissimilar emitter and base materials
  • Highly doped base
  • Dual B and C contacts
  • Identify WB and RB

4
HETEROJUNCTION BIPOLAR TRANSISTORS
  • The major development in bipolar transistors
    (since 1990)
  • HBTs break the link between NB and ?
  • Do this by making different barrier heights for
    electrons and holes
  • NB can reach 1E20cm-3

- this allows reduction of both WB and RB
SHBT
- this improves fT and fmax
  • Key feature is the wide-bandgap emitter

An example of Bandgap Engineering
5
Selecting an emitter for a GaAs base
AlGaAs / GaAs
InGaP / GaAs
6
InGaP/GaAs and AlGaAs/GaAs
Draw band diagrams for different ?emitter
7
Preparing to compute IC
  • Why do we show asymmetrical hemi-Maxwellians?

8
Current in a hemi-Maxwellian
Full Maxwellian distribution
Counter-propagating hemi-M's for n01E19/cm3
What is the current?
/1E20
9
Density of states
Recall
In 1-D, a state occupies how much k-space? What
is the volume in 3-D?
If kx and ky (and kz in 3-D) are large enough,
k-space is approximately spherical
Divide by V (volume) to get states/m3 Use
parabolic E-k (involves m) to get dE/dk Divide
by dE to get states/m3/eV
10
Velocities
Turn n(E) from previous slide into n(v) dv using

? vR 1E7 cm/s for GaAs
Currents associated with hemi-M's and M's
What is Je,total ?
1E7 A/cm2 for n06E18 /cm3
11
Collector current boundary conditions
12
Reduce our equation-set for the electron current
in the base
What about the recombination term?
13
Diffusion and Recombination in the base
Here, we need
In modern HBTs WB/Le ltlt 1 ?
and
is constant
14
Collector current controlling velocities

Diffusion (and no recombination) in the base
-1
Note - the reciprocal velocities - inclusion of
vR necessary in modern HBTs
Gives limit to validity of SLJ
15
Comparing results
  • What are the reasons for the difference?

16
Base current components
(iv)
  • Which IB components do we need to consider?

17
Base current components and Gummel plot
IC
IC (A/cm2)
IB (recombination)
IB (injection)
VBE (V)
  • What is the DC gain?

18
Preparing for the high-frequency analysis
  • Make all these functions of time and solve!
  • Or, use the quasi-static approximation

19
The Quasi-Static Approximation
q(x, y, z, t' ) f( VTerminals, t') q(x, y, z,
t' ) ? f( VTerminals, t lt t')
20
Small-signal circuit components
gm transconductance go output conductance
g? input conductance g12 reverse feedback
conductance
21
Recall g12dIb/dVce
next
22
Small-signal hybrid-? equivalent circuit
What are the parasitics?
23
HBT Parasitics
  • CEB and RB2 need explanation

24
Base-spreading resistance
y
25
Capacitance
Generally
1
Specifically
2
26
Emitter-base junction-storage capacitance
E
B
C
WB2
QNB
QNE
QNC
WB1

?VBE
  • ?QE,j is the change in charge entering the
    device through the emitter and creating the new
    width of the depletion layer (narrowing it in
    this example),
  • in response to a change in VBE (with E C at AC
    ground).
  • It can be regarded as a parallel-plate cap.

What is the voltage dependence of this cap?
27
Emitter-base base-storage capacitance concept
E
B
C
QNB
QNE
QNC

?VBE
  • ?QE,b is the change in charge entering the
    device through the emitter and resting in the
    base (the black electrons),
  • in response to a change in VBE (with E C at AC
    ground).
  • Its not a parallel-plate cap, and we only count
    one carrier.

28
Emitter-base base-storage capacitance evaluation
B
QNB
For the case of no recombination in the base
n(x)
n(WB)
x
WB
What is the voltage dependence of CEB,b ?
29
Base-emitter transit capacitance evaluation
Q 3q qe -2q
  • What are q0 and qd ?
  • Where do they come from ?

30
fT from hybrid-pi equivalent circuit
  • g0 and g? set to 0
  • fT is measured under AC short-circuit conditions.
  • We seek a solution for ic/ib2 that has a
    single-pole roll-off with frequency.
  • Why?
  • Because we wish to extrapolate at -20 dB/decade
    to unity gain.

31
Extrapolated fT
  • Assumption
  • Conditions
  • Current gain
  • Extrapolated fT

32
  • III-V for high gm
  • Implant isolation to reduce C?
  • Highly doped sub-collector and supra-emitter to
    reduce Rec
  • Dual contacts to reduce Rc
  • Lateral shrinking to reduce C's

33
Designing for high fT values
Why do collector delays dominate ?
34
How does Si get-in on the act?
35
Developing an expression for fmax
Assumption and conditions
36
Improving fmax
  • Pay even more attention to Rb and C?

Final HF question How far behind are Si MOSFETs?
37
HF MOS
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