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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-1
Lecture 13 - p-n Junction
March 7, 2007
Contents:
1. Ideal p-n junction in equilibrium
2. Ideal p-n junction out of equilibrium
Reading assignment:
del Alamo, Ch. 7, §§7.1, 7.2 (7.2.1, 7.2.2)
Announcements:
Quiz 1: March 13, 7:30-9:30 PM; lec-tures #1-12
(up to SCR-type transport). Open book.
Calculator required.
Final Exam scheduled: May 23, 1:30-3:30 PM.
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-2
Key questions
• What happens if you bring into intimate contact an n-type region
and a p-type region?
• What happens to the electrostatics of a p-n junction if one applies
a bias accross?
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-3
Motivation: pn junctions everywhere!
Example: CMOS
PMOS
n+
p+
n
NMOS
p+
n+
n+
p+
p
n
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-4
1. Ideal p-n junction in equilibrium
Eo
Eo
WSp
WSn
EFn
EFp
a) two semiconductors�
far apart
Eo
Eo
WSp
WSn
EFn
EFp
b) two semiconductors �
just before contact
Eo
qφbi
WSp
WSn
EF
c) two semiconductors �
in intimate contact
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
p
Lecture 13-5
n
Eo
Eo
χ
WSp
Ec
WSn
χ
Ec
EF
EF
Ev
Ev
Eo
qφbi
χ
WSp
Eo
Ec
WSn
χ
Ec
EF
Ev
Ev
qφbi = WSp − WSn = (EC − EF )|x�0 − (EC − EF )|x�0
no (x � 0)
= kT ln
no (x � 0)
Then:
φbi =
kT ND NA
ln
q
n2i
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-6
r
qND
0
x
0
-qNA
e
0
0
x
0
x
metallurgical junction
p
- - - -- - -- -
emax
n
+ + ++
+ ++
+ +
+ + ++
+
dipole of charge
f
0
fbi
log po, no
NA
ND
po
no
ni2
ND
ni2
NA
0
x
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-7
r
depletion approximation
exact
qND
-xp
0
xn
0
x
-qNA
e
xn
-xp
0
x
0
metallurgical junction
p
-
- - - --
emax
n
+ + ++
+ +
+ + +
+ + ++
+
dipole of charge
f
0
fbi
-xp
xn
0
x
log po, no
NA
ND
po
no
ni2
ND
ni2
NA
0
x
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-8
Do depletion approximation:
� Volume charge density:
ρ(x)
ρ(x)
ρ(x)
ρ(x)
�
�
�
�
0
−qNA
qND
0
in p-QNR: x < −xp
in SCR: − xp < x < 0
in SCR: 0 < x < xn
in n-QNR: xn < x
� Electric field:
E(x) � 0
qNA
(x + xp)
�
qND
E(x) �
(x − xn)
�
E(x) � 0
E(x) � −
in p-QNR: x ≤ −xp
in SCR: − xp ≤ x ≤ 0
in SCR: 0 ≤ x ≤ xn
in n-QNR: xn ≤ x
� Electrostatic potential [select φ(x = 0) = 0]:
φ(x) �
φ(x) �
φ(x) �
φ(x) �
qNAx2p
−
2�
qNA 2
(x + 2xpx)
2�
qND 2
−
(x − 2xnx)
2�
qND x2
n
2�
in p-QNR: x ≤ −xp
in SCR: − xp ≤ x ≤ 0
in SCR: 0 ≤ x ≤ xn
in n-QNR: xn ≤ x
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-9
Two unknowns: xn and xp .
• demand overall charge neutrality:
qNA xp = qND xn
• potential difference across structure must be φbi:
qND x
2n
qNA x
2
p
φ(xn) − φ(−xp)
=
+
=
φbi
2�
2�
Solve for xn and xp :
xn =
�
�
�
�
�
�
2�NA φbi
qND (ND + NA )
xp =
�
�
�
�
�
�
2�ND φbi
qNA(ND + NA )
Total SCR width:
xSCR =
�
�
�
�
�
�
2�(ND + NA)φbi
qNAND
Maximum electric field:
|Emax| =
�
�
�
�
�
�
2qNA ND φbi
�(ND + NA )
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-10
• symmetric junction: NA = ND :
xp = xn
|φ(−xp)| = φ(xn)
• asymmetric junction: i.e. NA > ND :
xp < xn
|φ(−xp)| < φ(xn)
• strongly asymmetric junction: i.e. p+-n junction NA � ND :
xp � xn � xSCR �
|Emax| �
�
�
�
�
�
�
�
�
�
�
2�φbi
qND
2qND φbi
�
the lowly-doped side controls everything
|φ(−xp)| � φ(xn) � φbi
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-11
ρ
qND
0
0
xSCR
x
ε
xSCR
0
0
x
εmax
φ
φbi
0
0
xSCR
x
Ec
EF
Ev
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-12
2. Ideal p-n junction out of equilibrium
Apply voltage across:
• forward bias: p-region positive with respect to n-region
• reverse bias: p-region negative with respect to n-region
Voltage can drop in five distinct regions:
• ohmic contact to n-region
• quasi-neutral n-region
• space-charge region
• quasi-neutral p-region
• ohmic contact to p-region
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-13
� Electrostatics
Battery grabs on majority carrier Fermi levels [will see when we
discuss ohmic contacts].
Application of voltage splits Fermi levels:
Ec
qφbi
EF
Ev
p
n
Ec
q(φbi-V)
Efn
V
qV
Efp
Ev
Ec
q(φbi-V)
Efp
qV
Efn
Ev
In forward and reverse bias:
φbi → φbi − V
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-14
Qualitatively, electrostatics unchanged out of equilibrium, but SCR
widens and shrinks, as needed:
ρ
qND
-xp(V)
0
0
xn(V)
x
V>0
V=0
-qNA
V<0
ε
0
0
x
0
x
εmax(V)
φ
0
φbi-V
φbi
φbi-V
→ use equilibrium equations:
xSCR(V ) =
�
�
�
�
�
�
|Emax(V )| =
�
�
�
�
�
2�(ND + NA )(φbi − V )
V
= xSCR(V = 0) 1 −
qNAND
φbi
�
�
�
�
�
�
�
�
�
�
�
2qNA ND (φbi − V )
V
= |Emax(V = 0)| 1 −
�(ND + NA)
φbi
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-15
� Depletion capacitance
Think differentially:
ρ
qND
ΔQ
+Q
-xp(V)
0
xn(V)
ΔQ
p
-
-Q
n
- - --- -- - -
+
+ + ++
+
++ +
+ + +
+ +
x
V
+
+
+
+
-qNA
V+ΔV
Δρ
+ΔQ
xn(V)
0
x
-xp(V)
−ΔQ
C(V ) =
�
xSCR(V )
Then:
C(V ) =
�
�
�
�
�
�
�qNA ND
C(V = 0)
= �
2(ND + NA)(φbi − V )
1 − φV
bi
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
C(V ) =
�
�
�
�
�
�
Lecture 13-16
�qNA ND
C(V = 0)
= �
2(ND + NA)(φbi − V )
1 − φV
bi
For p+-n junction:
C(V ) =
�
�
�
�
�
�
�qND
2(φbi − V )
Capacitance dominated by lowly-doped side
Technique to extract φbi and Nlow :
1
2(φbi − V )
=
C2
�qND
Q
1
C
C2
-
2
εqN
D
φbi
V
0
0
φbi V
0
φbi
V
C
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
MIT OpenCourseWare (http://ocw.mit.edu/), Massachusetts Institute of Technology. Downloaded on [DD Month YYYY].
6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-17
Experimental verification:
Fortini, A., A. Hairie, and M. Gomina. "Analysis and Capacitive Measurement of the Built-in-field Parameter in Highly Doped Emitters."
IEEE Transactions on Electron Devices 29, no. 10 (1982): 1604-1610. Copyright 1982 IEEE. Used with permission.
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
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6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007
Lecture 13-18
Key conclusions
• Built-in potential of p-n junction:
φbi =
kT ND NA
ln
q
n2i
• Depletion approximation: two quasi-neutral regions separated
by a space-charge region.
• In strongly asymmetric junction electrostatics dominated by re­
gion with lowest doping level; i.e. for p+-n junction:
xSCR �
�
�
�
�
�
2�φbi
qND
|Emax| �
�
�
�
�
�
2qND φbi
�
• Electrostatics out of equilibrium same as in TE if φbi ⇒ φbi − V .
• Depletion capacitance due to SCR width modulation:
C(V ) =
�
xSCR(V )
Cite as: Jesús del Alamo, course materials for 6.720J Integrated Microelectronic Devices, Spring 2007.
MIT OpenCourseWare (http://ocw.mit.edu/), Massachusetts Institute of Technology. Downloaded on [DD Month YYYY].
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