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Material Type: Exam; Professor: Bean; Class: Solid State Devices; Subject: Electrical and Computer Engineering; University: University of Virginia; Term: Spring 2009;
Typology: Exams
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Semiconductor Devices - Hour 30
BJT Example: Part II
(MCD: Entire Bipolar Calculation)
Last Time:
Started with the physical structure of a bipolar transistor
micron
4 −
cm⋅
Emitter
P Base
-^
Collector
Picked the doping of each layer:
d_E
19
cm
3
⋅
a_B
17
cm
3
⋅
d_C
(^15)
cm
3
Picked the full ("metallurgical") thickness of each layer:
0.2micron
0.2micron
250micron
Immediately ran into a problem - what are the "effective" layer thicknesses?
x
E_eff
x
B_eff
x
C_eff
EB
BC
1
Effective thicknesses depend on depletion layers - which depend on voltages applied to junctionsSo next I had decide how I was going to USE the transistor!
Chose:
its voltage drop => collector at ~ 5 volts
load
C
~ 5 volts
0 volts
Note, final choice (small load R) may not be good circuit sense but allowed me to simplify OUR problemV
applied_left
p_layer
n_layer
−
applied_right
p_layer
n_layer
−
0.5volt :=
volt
Signs on voltages are EXTREMELY important and follow from diagram and V
xy
x^
y
2
Choice 1: Complex hyperbolic equations with both V
BE
and V
BC
voltage factors (book/my earlier lectures):
Completely general
: Any layer thickness / Any junction bias
However:
A bear to use!
Choice 2: "Straight-line" approximations for emitter and base layers
Appropriate if
Emitter & base layers are << thinner than their minority carrier's diffusion length
E-B junction slightly forward biased / B-C junction strongly reverse biased
This is exactly what you will want anyway, if are trying to design an amplifying transistor!
So we WANT a transistor that will obey simpler equations - just need to check to see if we DO satisfy conditions:
Voltage bias conditions WERE chosen to satisfy requirements!Are our emitter and base layers thinner than diffusion lengths?
Had to fully evaluate parameters of MINORITY CARRIER in each layer:
4
Equilibrium minority carrier concentration is each layer is n
(^2) i / (majority carrier concentration):
p
no_C
n
(^2) i
n
no_C
=
p
no_E
n
(^2) i
n
no_E
=
n
po_B
n
(^2) i
p
po_B
=
p
no_E
cm
(^3)
n
po_B
(^3)
⋅^
cm
(^3)
p
no_C
(^5)
⋅^
cm
(^3)
Then to get minority carrier diffusion lengths ( L
τ⋅
) needed minority diffusivity and lifetime
Assumed for all minority carriers:
τ
6 −
sec⋅
To get the diffusivities, used Einstein's Relationship:
D μ
k T
⋅ q
=
For which we needed the minority carrier mobilities in each layer - based on ion concentration in each layer:
Emitter
Base
Collector
d_E
(^19)
cm
(^3)
a_B
(^17)
cm
(^3)
d_C
(^15)
cm
(^3)
Doping = Ions:
5
P in emitter
N in base
P in collector
Ions = donor / acceptor that created MAJORITY CARRIERS
(^19)
⋅^
cm
(^3)
emitter
(^17)
⋅^
cm
(^3)
base
(^15)
⋅^
cm
(^3)
collector
Does this minority stuff make sense yet?Should we go over more carefully or are you content w/ screwing up on final?
Used mobilities and Einstein Relationship to get minority carrier diffusivities for each layer:
p_E
μ
p_E
k T
⋅ q
n_B
μ
n_B
k T
⋅ q
p_C
μ
p_C
k T
⋅ q
p_E
cm
(^2) sec
n_B
cm
(^2) sec
p_C
cm
(^2) sec
Which finally yielded the minority carrier diffusion lengths:
7
p_E
p_E
τ⋅
n_B
n_B
τ⋅
p_C
p_C
τ⋅
p_E
13.461 micron
n_B
45.539 micron
p_C
34.435 micron
Which we compared with the layer's effective thicknesses:
x
E_eff
0.199 micron
x
B_eff
0.1 micron
x
C_eff
247.42 micron
For emitter and base:
Effective layer thickness ARE << minority diffusion lengths
For collector:
Effective thickness >> minority diffusion length
Use Straight lines
Use exponential / hyperbolic
For the minority carrier profiles in NPN bipolar transistor (from later part of lecture 27):
δ
p
nE
x( )
p
no_E
e
q V
BE ⋅^ k T
⋅^
x
x −
x
E_eff ⋅
Emitter
Base
δ
n
pB
x( )
n
po_B
e
q V
BE ⋅^ k T
⋅^
x
x' −
x
B_eff
⋅^
x' x
B_eff
−
8
Mathcad input:
P-Base
q
19 −
coul
N-Emitter
eV
q volt
N-Collector
k
5 −
⋅^
eVK
p
n_E
x( )
p
no_E
e
q V
BE ⋅^ k T
⋅
x
E_eff
Diffusion current = - (charge) * Diffusivity * (concentration gradient)
pE
q D
p_E ⋅^
p
no_E ⋅
x
E_eff
e
q V
BE ⋅^ k T
⋅
pE
5 −
cm
(^2)
Holes flowing into thin emitter N-emitter
of an NPN bipolar transistor
10
P-Base
N-Emitter
N-Collector
n
po_B
e
q V
BE ⋅^ k T
⋅
n
p_B
x( )
x
B_eff
Recombination = Total stored minority charge / minority lifetime:
q x
B_eff ⋅^
n
po_B ⋅ 2
τ⋅^
e
q V
BE ⋅^ k T
⋅
7 −
cm
(^2)
Electrons recombining in thin base
of an NPN bipolar transistor
11
Which in the thin base / low recombination / straight-line model this is ~ J
nC
nC
nE
:=
P-Base
N-Emitter
N-Collector
δ
p
n_C
p
no_C
e
x − L p_C
⋅
Which plugging slope into diffusion current expression gives:
pC
q D
p_C ⋅^
p
no_C ⋅ L
p_C
pC
10 −
cm
(^2)
Holes flowing out of a thick collector
13
Summarizing our calculated currents for this transistor with our choices of operating voltages:
nE
cm
(^2)
7 −
cm
(^2)
nC
cm
(^2)
pE
5 −
cm
(^2)
pC
10 −
cm
(^2)
Can now calculate this transistor's operating parameters (
with
our choices of voltages)
α
T
= "Base Transport Factor" = fraction of minority carriers making it across the base:
14
nC
6 −
α
T
= 1 - 2.411 x 10
"Common-Emitter" Current Gain:
nE
nC
nE
pE
nC
pC
pE
pE
pC −
pC
β
p_E
a_B ⋅^
x
B_eff ⋅
n_B
d_E ⋅^
x
E_eff ⋅
x B_effLn_B
2
Calculating from the formula:
16
β
p_E
a_B ⋅^
x
B_eff ⋅
n_B
d_E ⋅^
x
E_eff ⋅
x
B_effLn_B
2
We have a pretty high gaintransistor!!
β
(^3)
Calculating from currents:
β
nC
pC
pE
pC −
β
nC
pC
pE
pC −
β
(^3)
γ^
"Emitter Injection Efficiency" = desirable E-B current / all E-B current
nE
Don't want J
pE
because adds to J
B
input I must provide
pE
17