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Course: Electronic Devices
paper code: EC301
Course Coordinator: Arpan Deyasi
Department of Electronics and Communication Engineering
RCC Institute of Information Technology
Kolkata, India
8/27/2020 1Arpan Deyasi, RCCIIT, India
Topic: p-n Junction-II
Classification of p-n junction based on doping profile
Abrupt Linearly-graded
ND
NA
zn
-zp
ND
NA
W/2
-W/2
W
8/27/2020 2Arpan Deyasi, RCCIIT, India
D n A pN z N z=
Electrical Properties of Abrupt Junction
From charge neutrality condition
Total depletion width
n pz z W+ =
8/27/2020 3Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
A
n
D A
N
z W
N N
=
+
D
p
D A
N
z W
N N
=
+
8/27/2020 4Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
From Poisson’s equation
dE
dz
ρ
ε
=
n DqNρ =
p AqNρ = −
D AdE qN qN
dz ε ε
= = −
8/27/2020 5Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
D AqN qN
E dz dz
ε ε
= = −∫ ∫
1 2
D AqN qN
E z C z C
ε ε
= + =− +
8/27/2020 6Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
at z = zn , E = 0 1
D
n
qN
C z
ε
= −
( )D
n
qN
E z z
ε
=− −
at z =-zp , E = 0 2
A
p
qN
C z
ε
= −
( )A
p
qN
E z z
ε
=− +
8/27/2020 7Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
Maximum electric field
max
D A
n p
qN qN
E z z
ε ε
=− =−
max . . . .D A A D
D A D A
qN N qN N
E W W
N N N Nε ε
=− =−
+ +
8/27/2020 8Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
8/27/2020 9Arpan Deyasi, RCCIIT, India
Junction potential
n
p
z
j
z
V Edz
−
= − ∫
0
0
n
p
z
j
z
V Edz Edz
−
=− −∫ ∫
8/27/2020 10Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
0
0
( ) ( )
n
p
z
A D
j p n
z
qN qN
V z z dz z z dz
ε ε−
= + + −∫ ∫
2 2
2 2
A D
j p n
qN qN
V z z
ε ε
= +
8/27/2020 11Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
2 2
2 2
A D D A
j
D A D A
qN N qN N
V W W
N N N Nε ε
   
+   
+ +   
2
2
D A
j
D A
q N N
V W
N Nε
 
=  
+ 
8/27/2020 12Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
Depletion width
1/2
2 D A
j
D A
N N
W V
q N N
ε  +
=   
  
For externally applied voltage VA
1/2
2
( )D A
j A
D A
N N
W V V
q N N
ε  +
−  
  
8/27/2020 13
Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
Depletion Capacitance
Wp n
8/27/2020 14Arpan Deyasi, RCCIIT, India
j
j
dQ
C
dV
=
Electrical Properties of Abrupt Junction
D n A pQ V qN Az qN Azρ= = =
where
A
D
D A
WN
Q qN A
N N
=
+
8/27/2020 15Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
1/2
2A D A
D j
D A D A
N N N
Q qN A V
N N q N N
ε  +
=   
+   
1/2
2
2 D A
j
D A
N N
Q qA V
N N
ε
  
=   
+  
8/27/2020 16Arpan Deyasi, RCCIIT, India
Electrical Properties of Abrupt Junction
1/2
2
2
D A
j
j D A
qA N N
C
V N N
ε  
=   
+   
j
A
C
W
ε
=
8/27/2020 17Arpan Deyasi, RCCIIT, India
Electrical Properties of Linear-Graded Junction
From Poisson’s equation
dE
dz
ρ
ε
=
where kzqρ =
dE kzq
dz ε
=
8/27/2020 Arpan Deyasi, RCCIIT, India 18
Electrical Properties of Linear-Graded Junction
kzq
E dz
ε
= ∫
2
1.
2
kq z
E C
ε
= +
8/27/2020 Arpan Deyasi, RCCIIT, India 19
Electrical Properties of Linear-Graded Junction
at z = ±W/2, E = 0
2
1 .
8
kq z
C
ε
= −
2
2
2 4
kq W
E z
ε
 
=− − 
 
8/27/2020 Arpan Deyasi, RCCIIT, India 20
Electrical Properties of Linear-Graded Junction
at z = 0, E = Emax
2
max
8
kq
E W
ε
= −
8/27/2020 Arpan Deyasi, RCCIIT, India 21
Electrical Properties of Linear-Graded Junction
Junction potential
/2
/2
W
j
W
V Edz
−
= − ∫
/2 2
2
/2
2 4
W
j
W
kq W
V z dz
ε−
 
= − 
 
∫
8/27/2020 Arpan Deyasi, RCCIIT, India 22
Electrical Properties of Linear-Graded Junction
3
12
j
qk
V W
ε
=
Depletion width
1/3
12 jV
W
qk
ε 
=  
 
8/27/2020 Arpan Deyasi, RCCIIT, India 23
Electrical Properties of Linear-Graded Junction
Depletion Capacitance
j
j
dQ
C
dV
=
where
dQ A dz Aqkzdzρ= =
/2 2
0
8
W
qAkW
Q A qkzdz= =∫
8/27/2020 Arpan Deyasi, RCCIIT, India 24
Electrical Properties of Linear-Graded Junction
2/3
12
8
jVqAk
Q
qk
ε 
=  
 
1/3
2
12
j
j
qk
C A
V
ε 
=   
 
8/27/2020 25
Arpan Deyasi, RCCIIT, India
Wp n
Diffusion Capacitance (for Abrupt and Linear-graded)
8/27/2020 Arpan Deyasi, RCCIIT, India 26
Diffusion Capacitance (for Abrupt and Linear-graded)
Diode current due to holes
0 exp 1p
n
p T
AqD V
I p
L V
  
−  
  
If applied voltage is high
0 expp
n
p T
AqD V
I p
L V
 
=  
 
8/27/2020 Arpan Deyasi, RCCIIT, India 27
Diffusion Capacitance (for Abrupt and Linear-graded)
Charge stored at the junction due to holes
pQ Iτ=
0 expp
n p
p T
AqD V
Q p
L V
τ
 
=  
 
0 expp n
T
V
Q AqL p
V
 
=  
 
8/27/2020 Arpan Deyasi, RCCIIT, India 28
Diffusion Capacitance (for Abrupt and Linear-graded)
T
dQ
C
dV
=
0 expT p n
T
d V
C AqL p
dV V
  
=   
  
0
exp
p n
T
T T
AqL p V
C
V V
 
=  
 
8/27/2020 Arpan Deyasi, RCCIIT, India 29
Diffusion Capacitance (for Abrupt and Linear-graded)
0
exp
n p
T
T T
AqL n V
C
V V
 
=  
 
If we consider electron current

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Electrical properties of p-n junction

  • 1. Course: Electronic Devices paper code: EC301 Course Coordinator: Arpan Deyasi Department of Electronics and Communication Engineering RCC Institute of Information Technology Kolkata, India 8/27/2020 1Arpan Deyasi, RCCIIT, India Topic: p-n Junction-II
  • 2. Classification of p-n junction based on doping profile Abrupt Linearly-graded ND NA zn -zp ND NA W/2 -W/2 W 8/27/2020 2Arpan Deyasi, RCCIIT, India
  • 3. D n A pN z N z= Electrical Properties of Abrupt Junction From charge neutrality condition Total depletion width n pz z W+ = 8/27/2020 3Arpan Deyasi, RCCIIT, India
  • 4. Electrical Properties of Abrupt Junction A n D A N z W N N = + D p D A N z W N N = + 8/27/2020 4Arpan Deyasi, RCCIIT, India
  • 5. Electrical Properties of Abrupt Junction From Poisson’s equation dE dz ρ ε = n DqNρ = p AqNρ = − D AdE qN qN dz ε ε = = − 8/27/2020 5Arpan Deyasi, RCCIIT, India
  • 6. Electrical Properties of Abrupt Junction D AqN qN E dz dz ε ε = = −∫ ∫ 1 2 D AqN qN E z C z C ε ε = + =− + 8/27/2020 6Arpan Deyasi, RCCIIT, India
  • 7. Electrical Properties of Abrupt Junction at z = zn , E = 0 1 D n qN C z ε = − ( )D n qN E z z ε =− − at z =-zp , E = 0 2 A p qN C z ε = − ( )A p qN E z z ε =− + 8/27/2020 7Arpan Deyasi, RCCIIT, India
  • 8. Electrical Properties of Abrupt Junction Maximum electric field max D A n p qN qN E z z ε ε =− =− max . . . .D A A D D A D A qN N qN N E W W N N N Nε ε =− =− + + 8/27/2020 8Arpan Deyasi, RCCIIT, India
  • 9. Electrical Properties of Abrupt Junction 8/27/2020 9Arpan Deyasi, RCCIIT, India Junction potential n p z j z V Edz − = − ∫ 0 0 n p z j z V Edz Edz − =− −∫ ∫
  • 10. 8/27/2020 10Arpan Deyasi, RCCIIT, India Electrical Properties of Abrupt Junction 0 0 ( ) ( ) n p z A D j p n z qN qN V z z dz z z dz ε ε− = + + −∫ ∫ 2 2 2 2 A D j p n qN qN V z z ε ε = +
  • 11. 8/27/2020 11Arpan Deyasi, RCCIIT, India Electrical Properties of Abrupt Junction 2 2 2 2 A D D A j D A D A qN N qN N V W W N N N Nε ε     +    + +    2 2 D A j D A q N N V W N Nε   =   + 
  • 12. 8/27/2020 12Arpan Deyasi, RCCIIT, India Electrical Properties of Abrupt Junction Depletion width 1/2 2 D A j D A N N W V q N N ε  + =       For externally applied voltage VA 1/2 2 ( )D A j A D A N N W V V q N N ε  + −     
  • 13. 8/27/2020 13 Arpan Deyasi, RCCIIT, India Electrical Properties of Abrupt Junction Depletion Capacitance Wp n
  • 14. 8/27/2020 14Arpan Deyasi, RCCIIT, India j j dQ C dV = Electrical Properties of Abrupt Junction D n A pQ V qN Az qN Azρ= = = where A D D A WN Q qN A N N = +
  • 15. 8/27/2020 15Arpan Deyasi, RCCIIT, India Electrical Properties of Abrupt Junction 1/2 2A D A D j D A D A N N N Q qN A V N N q N N ε  + =    +    1/2 2 2 D A j D A N N Q qA V N N ε    =    +  
  • 16. 8/27/2020 16Arpan Deyasi, RCCIIT, India Electrical Properties of Abrupt Junction 1/2 2 2 D A j j D A qA N N C V N N ε   =    +    j A C W ε =
  • 17. 8/27/2020 17Arpan Deyasi, RCCIIT, India Electrical Properties of Linear-Graded Junction From Poisson’s equation dE dz ρ ε = where kzqρ = dE kzq dz ε =
  • 18. 8/27/2020 Arpan Deyasi, RCCIIT, India 18 Electrical Properties of Linear-Graded Junction kzq E dz ε = ∫ 2 1. 2 kq z E C ε = +
  • 19. 8/27/2020 Arpan Deyasi, RCCIIT, India 19 Electrical Properties of Linear-Graded Junction at z = ±W/2, E = 0 2 1 . 8 kq z C ε = − 2 2 2 4 kq W E z ε   =− −   
  • 20. 8/27/2020 Arpan Deyasi, RCCIIT, India 20 Electrical Properties of Linear-Graded Junction at z = 0, E = Emax 2 max 8 kq E W ε = −
  • 21. 8/27/2020 Arpan Deyasi, RCCIIT, India 21 Electrical Properties of Linear-Graded Junction Junction potential /2 /2 W j W V Edz − = − ∫ /2 2 2 /2 2 4 W j W kq W V z dz ε−   = −    ∫
  • 22. 8/27/2020 Arpan Deyasi, RCCIIT, India 22 Electrical Properties of Linear-Graded Junction 3 12 j qk V W ε = Depletion width 1/3 12 jV W qk ε  =    
  • 23. 8/27/2020 Arpan Deyasi, RCCIIT, India 23 Electrical Properties of Linear-Graded Junction Depletion Capacitance j j dQ C dV = where dQ A dz Aqkzdzρ= = /2 2 0 8 W qAkW Q A qkzdz= =∫
  • 24. 8/27/2020 Arpan Deyasi, RCCIIT, India 24 Electrical Properties of Linear-Graded Junction 2/3 12 8 jVqAk Q qk ε  =     1/3 2 12 j j qk C A V ε  =     
  • 25. 8/27/2020 25 Arpan Deyasi, RCCIIT, India Wp n Diffusion Capacitance (for Abrupt and Linear-graded)
  • 26. 8/27/2020 Arpan Deyasi, RCCIIT, India 26 Diffusion Capacitance (for Abrupt and Linear-graded) Diode current due to holes 0 exp 1p n p T AqD V I p L V    −      If applied voltage is high 0 expp n p T AqD V I p L V   =    
  • 27. 8/27/2020 Arpan Deyasi, RCCIIT, India 27 Diffusion Capacitance (for Abrupt and Linear-graded) Charge stored at the junction due to holes pQ Iτ= 0 expp n p p T AqD V Q p L V τ   =     0 expp n T V Q AqL p V   =    
  • 28. 8/27/2020 Arpan Deyasi, RCCIIT, India 28 Diffusion Capacitance (for Abrupt and Linear-graded) T dQ C dV = 0 expT p n T d V C AqL p dV V    =       0 exp p n T T T AqL p V C V V   =    
  • 29. 8/27/2020 Arpan Deyasi, RCCIIT, India 29 Diffusion Capacitance (for Abrupt and Linear-graded) 0 exp n p T T T AqL n V C V V   =     If we consider electron current