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Shockley Diode & SCR
Arpan Deyasi
Dept of ECE, RCCIIT, Kolkata, India
12/27/2020 1Arpan Deyasi, RCCIIT
12/27/2020 2Arpan Deyasi, RCCIIT
p n p n
Shockley Diode
P-N-P-N diode
named after William Shockley
Four layer device
Three junctions
12/27/2020 Arpan Deyasi, RCCIIT 3
Shockley Diode
p n p n
J1 J2 J3
J1, J3: forward biased
J2: reverse biased
12/27/2020 Arpan Deyasi, RCCIIT 4
p
n
p
n
p
n
p
n
p
n
Equivalent Structure
12/27/2020 Arpan Deyasi, RCCIIT 5
n
p
n
p
n
p
Q1
Q1
Q2
Q2
Equivalent Circuit
12/27/2020 Arpan Deyasi, RCCIIT 6
Q1
Q2
IA
IEP
IBP
ICP
IBN
IA
ICN
IEN
IA: Anode current
or total current
Current components in Equivalent Circuit
12/27/2020 Arpan Deyasi, RCCIIT 7
For any BJT
C E COI I Iα= +
CN N EN CONI I Iα= +
CP P EP COPI I Iα= +Q1:
Q2:
Analysis
12/27/2020 Arpan Deyasi, RCCIIT 8
IA
IEP
IBP
ICP
IBN
Q1
Q2
IA
ICN
IEN
CP P EP COPI I Iα= +
Analysis
EP BP P EP COPI I I Iα− = +
EP P EP COP BPI I I Iα= + +
12/27/2020 Arpan Deyasi, RCCIIT 9
A EPI I=
IA
IEP
IBP
ICP
IBN
Q1
Q2
IA
ICN
IEN
Analysis
EP P EP COP BPI I I Iα= + +
A P A COP BPI I I Iα= + +
(1 )A P COP BPI I Iα− = +
12/27/2020 Arpan Deyasi, RCCIIT 10
Analysis
IA
IEP
IBP
ICP
IBN
Q1
Q2
IA
ICN
IEN
BP CNI I=
(1 )A P COP BPI I Iα− = +
(1 )A P COP CNI I Iα− = +
(1 )A P COP N EN CONI I I Iα α− = + +
12/27/2020 Arpan Deyasi, RCCIIT 11
Analysis
EN AI I=
IA
IEP
IBP
ICP
IBN
Q1
Q2
IA
ICN
IEN
(1 )A P COP
N EN CON
I I
I I
α
α
− = +
+
(1 )A P COP N A CONI I I Iα α− = + +
12/27/2020 Arpan Deyasi, RCCIIT 12
Analysis IA
IEP
IBP
ICP
IBN
Q1
Q2
IA
ICN
IEN
(1 )A P N
COP CON
I
I I
α α− −
= +
(1 )A P N COI Iα α− − =
(1 )
CO
A
P N
I
I
α α
=
− −
12/27/2020 Arpan Deyasi, RCCIIT 13
Analysis
(1 )
CO
A
P N
I
I
α α
=
− −
low supply condition ( ) 1P Nα α+ <<
Forward blocking state / OFF state
A COI I≈
12/27/2020 Arpan Deyasi, RCCIIT 14
Analysis
(1 )
CO
A
P N
I
I
α α
=
− −
low supply condition ( ) 1P Nα α+ <<
Forward blocking state / OFF state
A COI I≈
12/27/2020 Arpan Deyasi, RCCIIT 15
Analysis
(1 )
CO
A
P N
I
I
α α
=
− −
high supply condition ( ) 1P Nα α+ 
Forward breakdown state / ON state
AI ∞
12/27/2020 Arpan Deyasi, RCCIIT 16
I-V characteristics of Shockley Diode
VAKFVAKR
IAF
IAR
Diode region
Unstable region
Reverse
bias region
VBR
ICO
0.7 V
IL
IH
12/27/2020 Arpan Deyasi, RCCIIT 17
Drawbacks of Shockley Diode
Electrical length of unstable region is very long
Q: How to reduce it?
VBR should be lowered
Solution: Shockley diode with additional bias
12/27/2020 Arpan Deyasi, RCCIIT 18
I-V characteristics of Shockley Diode
VAKFVAKR
IAF
IAR
Unstable region
VBR
0.7 V
(VJ1+VJ3-VJ2) < 2.1 V
12/27/2020 Arpan Deyasi, RCCIIT 19
Modified Shockley Diode
p n p n
J1 J2 J3
Silicon
Controlled
Rectifier
12/27/2020 Arpan Deyasi, RCCIIT 20
I-V characteristics of SCR
VAKFVAKR
IAF
IAR
Unstable region
VBR
0.7 V
VBR1
VBR2VBR3
12/27/2020 Arpan Deyasi, RCCIIT 21
1P Nα α+ =
1
1 1
NP
P N
ββ
β β
+ =
+ +
1P Nβ β =
Characteristic Equation of SCR

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Shockley Diode & SCR

  • 1. Shockley Diode & SCR Arpan Deyasi Dept of ECE, RCCIIT, Kolkata, India 12/27/2020 1Arpan Deyasi, RCCIIT
  • 2. 12/27/2020 2Arpan Deyasi, RCCIIT p n p n Shockley Diode P-N-P-N diode named after William Shockley Four layer device Three junctions
  • 3. 12/27/2020 Arpan Deyasi, RCCIIT 3 Shockley Diode p n p n J1 J2 J3 J1, J3: forward biased J2: reverse biased
  • 4. 12/27/2020 Arpan Deyasi, RCCIIT 4 p n p n p n p n p n Equivalent Structure
  • 5. 12/27/2020 Arpan Deyasi, RCCIIT 5 n p n p n p Q1 Q1 Q2 Q2 Equivalent Circuit
  • 6. 12/27/2020 Arpan Deyasi, RCCIIT 6 Q1 Q2 IA IEP IBP ICP IBN IA ICN IEN IA: Anode current or total current Current components in Equivalent Circuit
  • 7. 12/27/2020 Arpan Deyasi, RCCIIT 7 For any BJT C E COI I Iα= + CN N EN CONI I Iα= + CP P EP COPI I Iα= +Q1: Q2: Analysis
  • 8. 12/27/2020 Arpan Deyasi, RCCIIT 8 IA IEP IBP ICP IBN Q1 Q2 IA ICN IEN CP P EP COPI I Iα= + Analysis EP BP P EP COPI I I Iα− = + EP P EP COP BPI I I Iα= + +
  • 9. 12/27/2020 Arpan Deyasi, RCCIIT 9 A EPI I= IA IEP IBP ICP IBN Q1 Q2 IA ICN IEN Analysis EP P EP COP BPI I I Iα= + + A P A COP BPI I I Iα= + + (1 )A P COP BPI I Iα− = +
  • 10. 12/27/2020 Arpan Deyasi, RCCIIT 10 Analysis IA IEP IBP ICP IBN Q1 Q2 IA ICN IEN BP CNI I= (1 )A P COP BPI I Iα− = + (1 )A P COP CNI I Iα− = + (1 )A P COP N EN CONI I I Iα α− = + +
  • 11. 12/27/2020 Arpan Deyasi, RCCIIT 11 Analysis EN AI I= IA IEP IBP ICP IBN Q1 Q2 IA ICN IEN (1 )A P COP N EN CON I I I I α α − = + + (1 )A P COP N A CONI I I Iα α− = + +
  • 12. 12/27/2020 Arpan Deyasi, RCCIIT 12 Analysis IA IEP IBP ICP IBN Q1 Q2 IA ICN IEN (1 )A P N COP CON I I I α α− − = + (1 )A P N COI Iα α− − = (1 ) CO A P N I I α α = − −
  • 13. 12/27/2020 Arpan Deyasi, RCCIIT 13 Analysis (1 ) CO A P N I I α α = − − low supply condition ( ) 1P Nα α+ << Forward blocking state / OFF state A COI I≈
  • 14. 12/27/2020 Arpan Deyasi, RCCIIT 14 Analysis (1 ) CO A P N I I α α = − − low supply condition ( ) 1P Nα α+ << Forward blocking state / OFF state A COI I≈
  • 15. 12/27/2020 Arpan Deyasi, RCCIIT 15 Analysis (1 ) CO A P N I I α α = − − high supply condition ( ) 1P Nα α+  Forward breakdown state / ON state AI ∞
  • 16. 12/27/2020 Arpan Deyasi, RCCIIT 16 I-V characteristics of Shockley Diode VAKFVAKR IAF IAR Diode region Unstable region Reverse bias region VBR ICO 0.7 V IL IH
  • 17. 12/27/2020 Arpan Deyasi, RCCIIT 17 Drawbacks of Shockley Diode Electrical length of unstable region is very long Q: How to reduce it? VBR should be lowered Solution: Shockley diode with additional bias
  • 18. 12/27/2020 Arpan Deyasi, RCCIIT 18 I-V characteristics of Shockley Diode VAKFVAKR IAF IAR Unstable region VBR 0.7 V (VJ1+VJ3-VJ2) < 2.1 V
  • 19. 12/27/2020 Arpan Deyasi, RCCIIT 19 Modified Shockley Diode p n p n J1 J2 J3 Silicon Controlled Rectifier
  • 20. 12/27/2020 Arpan Deyasi, RCCIIT 20 I-V characteristics of SCR VAKFVAKR IAF IAR Unstable region VBR 0.7 V VBR1 VBR2VBR3
  • 21. 12/27/2020 Arpan Deyasi, RCCIIT 21 1P Nα α+ = 1 1 1 NP P N ββ β β + = + + 1P Nβ β = Characteristic Equation of SCR