Title: Heterojunction%20Bipolar%20Transistors
1 Heterojunction Bipolar Transistors for High-Frequ
ency Operation
Day 3A, May 29, 2008, Pisa
2Outline
- 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?
3Schematic of InGaP/GaAs HBT
- Epitaxial structure
- Dissimilar emitter and base materials
- Highly doped base
- Dual B and C contacts
4HETEROJUNCTION 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
5Selecting an emitter for a GaAs base
AlGaAs / GaAs
InGaP / GaAs
6InGaP/GaAs and AlGaAs/GaAs
Draw band diagrams for different ?emitter
7 Preparing to compute IC
- Why do we show asymmetrical hemi-Maxwellians?
8Current in a hemi-Maxwellian
Full Maxwellian distribution
Counter-propagating hemi-M's for n01E19/cm3
What is the current?
/1E20
9Density 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
10Velocities
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
12Reduce 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)
18Preparing for the high-frequency analysis
- Make all these functions of time and solve!
- Or, use the quasi-static approximation
19The Quasi-Static Approximation
q(x, y, z, t' ) f( VTerminals, t') q(x, y, z,
t' ) ? f( VTerminals, t lt t')
20Small-signal circuit components
gm transconductance go output conductance
g? input conductance g12 reverse feedback
conductance
21Recall g12dIb/dVce
next
22Small-signal hybrid-? equivalent circuit
What are the parasitics?
23 HBT Parasitics
- CEB and RB2 need explanation
24Base-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 ?
30fT 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
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
33Designing for high fT values
Why do collector delays dominate ?
34How does Si get-in on the act?
35Developing an expression for fmax
Assumption and conditions
36Improving fmax
- Pay even more attention to Rb and C?
Final HF question How far behind are Si MOSFETs?
37HF MOS
What is this?