Semiconductor Devices - Final Notes | ECE 3103, Exams of Solid State Physics

Material Type: Exam; Professor: Bean; Class: Solid State Devices; Subject: Electrical and Computer Engineering; University: University of Virginia; Term: Spring 2009;

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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 10 4cm:=
N+ Emitter P Base N- Collector
Picked the doping of each layer:
Nd_E 1019 1
cm3
:= Na_B 1017 1
cm3
:= Nd_C 1015 1
cm3
:=
Picked the full ("metallurgical") thickness of each layer:
0.2micron 0.2micron 250micron
Immediately ran into a problem - what are the "effective" layer thicknesses?
xE_eff = ? xB_eff = ? xC_eff = ?
WEB = ? WBC = ?
Semiconductor_Devices_30.xmcd 12/4/2009
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pf12

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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⋅

N

Emitter

P Base

N

-^

Collector

Picked the doping of each layer:

N

d_E

19

cm

3

N

a_B

17

cm

3

N

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

W

EB

W

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:

  • "Common emitter" amplifier circuit- Power supply voltage of 5 volts- Emitter-base forward bias of 0.5 volts- Small enough load resistor that could ignore

its voltage drop => collector at ~ 5 volts

  • 5 volts

R

load

C

B

~ 5 volts

E

  • 0.5 volts

0 volts

Note, final choice (small load R) may not be good circuit sense but allowed me to simplify OUR problemV

applied_left

V

p_layer

V

n_layer

V

BE

V

applied_right

V

p_layer

V

n_layer

V

BC

V

BE

0.5volt :=

V

BC

volt

Signs on voltages are EXTREMELY important and follow from diagram and V

xy

= V

x^

- V

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

AND

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

D

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

N

d_E

(^19)

×

cm

(^3)

N

a_B

(^17)

×

cm

(^3)

N

d_C

(^15)

×

cm

(^3)

Doping = Ions:

5

  1. Determine minority carrier TYPE:

P in emitter

N in base

P in collector

  1. Figure out ion concentration that causes scattering which controls mobility:

Ions = donor / acceptor that created MAJORITY CARRIERS

(^19)

⋅^

cm

(^3)

⋅^

emitter

(^17)

⋅^

cm

(^3)

⋅^

base

(^15)

⋅^

cm

(^3)

⋅^

collector

  1. Use correct curve in chart above (one for that TYPE carrier at that layer's ION concentration) Anonymous show of hands:

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:

D

p_E

μ

p_E

k T

⋅ q

D

n_B

μ

n_B

k T

⋅ q

D

p_C

μ

p_C

k T

⋅ q

D

p_E

cm

(^2) sec

D

n_B

cm

(^2) sec

D

p_C

cm

(^2) sec

Which finally yielded the minority carrier diffusion lengths:

7

L

p_E

D

p_E

τ⋅

L

n_B

D

n_B

τ⋅

L

p_C

D

p_C

τ⋅

L

p_E

13.461 micron

L

n_B

45.539 micron

L

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

E

x −

(^

x

E_eff ⋅

Emitter

Base

δ

n

pB

x( )

n

po_B

e

q V

BE ⋅^ k T

⋅^

x

B

x' −

(^

x

B_eff

⋅^

x' x

B_eff

8

  1. Emitter hole current:

Mathcad input:

P-Base

q

19 −

coul

N-Emitter

eV

q volt

N-Collector

k

5 −

⋅^

eVK

T

300K

p

n_E

x( )

p

no_E

e

q V

BE ⋅^ k T

x

E_eff

Diffusion current = - (charge) * Diffusivity * (concentration gradient)

J

pE

q D

p_E ⋅^

p

no_E ⋅

x

E_eff

e

q V

BE ⋅^ k T

J

pE

5 −

×

A

cm

(^2)

Holes flowing into thin emitter N-emitter

of an NPN bipolar transistor

  1. Electrons recombination inside the base:

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:

J

RB

q x

B_eff ⋅^

n

po_B ⋅ 2

τ⋅^

e

q V

BE ⋅^ k T

J

RB

7 −

×

A

cm

(^2)

Electrons recombining in thin base

of an NPN bipolar transistor

  1. Electrons flowing through the base:

11

Which in the thin base / low recombination / straight-line model this is ~ J

nC

J

nC

J

nE

:=

  1. Holes leaking in from collector:

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:

J

pC

q D

p_C ⋅^

p

no_C ⋅ L

p_C

J

pC

10 −

×

A

cm

(^2)

Holes flowing out of a thick collector

13

Summarizing our calculated currents for this transistor with our choices of operating voltages:

J

nE

A

cm

(^2)

J

RB

7 −

×

A

cm

(^2)

J

nC

A

cm

(^2)

J

pE

5 −

×

A

cm

(^2)

J

pC

10 −

×

A

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

J

RB

J

nC

6 −

×

α

T

= 1 - 2.411 x 10

"Common-Emitter" Current Gain:

J

nE

J

nC

J

RB

J

E

J

nE

J

pE

J

C

J

nC

J

pC

J

pE

J

B

J

pE

J

RB

J

pC −

J

pC

β

J

C

J

B

D

p_E

N

a_B ⋅^

x

B_eff ⋅

D

n_B

N

d_E ⋅^

x

E_eff ⋅

x B_effLn_B

2

Calculating from the formula:

16

β

D

p_E

N

a_B ⋅^

x

B_eff ⋅

D

n_B

N

d_E ⋅^

x

E_eff ⋅

x

B_effLn_B

2

We have a pretty high gaintransistor!!

β

(^3)

×

Calculating from currents:

β

J

C

J

B

J

nC

J

pC

J

pE

J

RB

J

pC −

β

J

nC

J

pC

J

pE

J

RB

J

pC −

β

(^3)

×

γ^

"Emitter Injection Efficiency" = desirable E-B current / all E-B current

J

nE

Don't want J

pE

because adds to J

B

input I must provide

J

pE

17