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Bipolar Junction
Transistor
Arpan Deyasi
Dept of ECE, RCCIIT, Kolkata, India
12/27/2020 Arpan Deyasi, RCCIIT 1
12/27/2020 Arpan Deyasi, RCCIIT 2
12/27/2020 Arpan Deyasi, RCCIIT
Emitter
. It supplies carrier (for NPN, electron; for PNP, hole)
. Most heavily doped area
Collector
. It collects carrier (for NPN, electron; for PNP, hole)
. lighter doped than emitter, heavier doped than base
3
Base
. It forms the p-n junctions both with collector and emitter
. less doped than both of the regions
. thinnest region
. BE junction is always forward-biased (npn)
. BC junction is always reverse-biased (npn)
12/27/2020 Arpan Deyasi, RCCIIT 4
Gain parameters of Transistor
CB current gain C
E
I
I
α =
12/27/2020 Arpan Deyasi, RCCIIT 5
‘α’ is close to 1 because
small fractions of injected electrons from emitter to base
are lost due to recombination with holes
small hole current is injected from base to emitter
hole current from collector to base is negligible
C EI I≤ 1α ≈
12/27/2020 Arpan Deyasi, RCCIIT 6
CE current gain
C
B
I
I
β =
Gain parameters of Transistor
C BI I
1β 
12/27/2020 Arpan Deyasi, RCCIIT 7
Relation between α and β
C C
B E C
I I
I I I
β= =
−
1
1
C
E
C
E
I
I
I
I
α
β
α
 
 
 = =
− 
− 
 
1
β
α
β
=
+
12/27/2020 Arpan Deyasi, RCCIIT 8
Gain parameters of Transistor
Injection efficiency is defined as
the fraction of emitter current
due to electron injection from emitter to base
1
1
nE nE
pEpE nE pE
nE
I I
II I I
I
γ= = =
+  
+  
 
pE nEI I 1γ ≈
12/27/2020 Arpan Deyasi, RCCIIT 9
Gain parameters of Transistor
Transport efficiency is defined as
the fraction of electrons
injected from emitter to base which reach the collector
1nC nE rec rec
T
nE nE nE
I I I I
I I I
α
−
= = = −
rec nEI I 1Tα ≈
Transport efficiency is also known as Transport Factor
12/27/2020 Arpan Deyasi, RCCIIT 10
Gain parameters of Transistor
Collection efficiency is defined as
the ratio of collector leakage current to electron leakage current
from base to collector in reverse biased base collector junction
1
nC pC pCC
nC nC nC
I I II
M
I I I
+
= = = +
pC nCI I 1M ≥
Collector efficiency is also known as Collector Multiplication Factor
12/27/2020 Arpan Deyasi, RCCIIT 11
Base-Width Modulation
variation in the width of the base in a bipolar transistor due
to a variation in the applied base-to-collector voltage
12/27/2020 Arpan Deyasi, RCCIIT 12
Base-Width Modulation
VBE < VCE1 << VCE2
Effective base width is reduced ---- Early effect
12/27/2020 Arpan Deyasi, RCCIIT 13
Base narrowing has two consequences that affect the
current:
There is a lesser chance for recombination within the
“smaller” base region
The current of minority carriers injected across the
emitter junction increases
Base-Width Modulation
Early Effect
12/27/2020 Arpan Deyasi, RCCIIT 14
To countervail the Early- effect is a lightly doping of the collector
region and a heavy doping of the emitter region
Base-Width Modulation
12/27/2020 Arpan Deyasi, RCCIIT 15
The CB current gain (α), taking into account the effective width of
the base quasi-neutral region (assuming γ=1) is then given by
Base-Width Modulation
2
1
1
2
eff
T
B
W
L
α α
 
= ≈ −  
 
CE current gain (β) can be approximated with
2
2
1
B
eff
L
W
α
β
α
 
= =   −  
12/27/2020 Arpan Deyasi, RCCIIT 16
Punch-through Breakdown
The punch-through breakdown occurs when the reverse-bias C-B
voltage is so large that the C-B and the E-B depletion regions merge
Punch-through voltage is usually much larger than the
avalanche breakdown voltage
12/27/2020 Arpan Deyasi, RCCIIT 17
Punch-through Breakdown

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Gain parameters of BJT

  • 1. Bipolar Junction Transistor Arpan Deyasi Dept of ECE, RCCIIT, Kolkata, India 12/27/2020 Arpan Deyasi, RCCIIT 1
  • 3. 12/27/2020 Arpan Deyasi, RCCIIT Emitter . It supplies carrier (for NPN, electron; for PNP, hole) . Most heavily doped area Collector . It collects carrier (for NPN, electron; for PNP, hole) . lighter doped than emitter, heavier doped than base 3 Base . It forms the p-n junctions both with collector and emitter . less doped than both of the regions . thinnest region . BE junction is always forward-biased (npn) . BC junction is always reverse-biased (npn)
  • 4. 12/27/2020 Arpan Deyasi, RCCIIT 4 Gain parameters of Transistor CB current gain C E I I α =
  • 5. 12/27/2020 Arpan Deyasi, RCCIIT 5 ‘α’ is close to 1 because small fractions of injected electrons from emitter to base are lost due to recombination with holes small hole current is injected from base to emitter hole current from collector to base is negligible C EI I≤ 1α ≈
  • 6. 12/27/2020 Arpan Deyasi, RCCIIT 6 CE current gain C B I I β = Gain parameters of Transistor C BI I 1β 
  • 7. 12/27/2020 Arpan Deyasi, RCCIIT 7 Relation between α and β C C B E C I I I I I β= = − 1 1 C E C E I I I I α β α      = = −  −    1 β α β = +
  • 8. 12/27/2020 Arpan Deyasi, RCCIIT 8 Gain parameters of Transistor Injection efficiency is defined as the fraction of emitter current due to electron injection from emitter to base 1 1 nE nE pEpE nE pE nE I I II I I I γ= = = +   +     pE nEI I 1γ ≈
  • 9. 12/27/2020 Arpan Deyasi, RCCIIT 9 Gain parameters of Transistor Transport efficiency is defined as the fraction of electrons injected from emitter to base which reach the collector 1nC nE rec rec T nE nE nE I I I I I I I α − = = = − rec nEI I 1Tα ≈ Transport efficiency is also known as Transport Factor
  • 10. 12/27/2020 Arpan Deyasi, RCCIIT 10 Gain parameters of Transistor Collection efficiency is defined as the ratio of collector leakage current to electron leakage current from base to collector in reverse biased base collector junction 1 nC pC pCC nC nC nC I I II M I I I + = = = + pC nCI I 1M ≥ Collector efficiency is also known as Collector Multiplication Factor
  • 11. 12/27/2020 Arpan Deyasi, RCCIIT 11 Base-Width Modulation variation in the width of the base in a bipolar transistor due to a variation in the applied base-to-collector voltage
  • 12. 12/27/2020 Arpan Deyasi, RCCIIT 12 Base-Width Modulation VBE < VCE1 << VCE2 Effective base width is reduced ---- Early effect
  • 13. 12/27/2020 Arpan Deyasi, RCCIIT 13 Base narrowing has two consequences that affect the current: There is a lesser chance for recombination within the “smaller” base region The current of minority carriers injected across the emitter junction increases Base-Width Modulation Early Effect
  • 14. 12/27/2020 Arpan Deyasi, RCCIIT 14 To countervail the Early- effect is a lightly doping of the collector region and a heavy doping of the emitter region Base-Width Modulation
  • 15. 12/27/2020 Arpan Deyasi, RCCIIT 15 The CB current gain (α), taking into account the effective width of the base quasi-neutral region (assuming γ=1) is then given by Base-Width Modulation 2 1 1 2 eff T B W L α α   = ≈ −     CE current gain (β) can be approximated with 2 2 1 B eff L W α β α   = =   −  
  • 16. 12/27/2020 Arpan Deyasi, RCCIIT 16 Punch-through Breakdown The punch-through breakdown occurs when the reverse-bias C-B voltage is so large that the C-B and the E-B depletion regions merge Punch-through voltage is usually much larger than the avalanche breakdown voltage
  • 17. 12/27/2020 Arpan Deyasi, RCCIIT 17 Punch-through Breakdown