 k A C t

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MSE 310/ECE 340
Electrical Properties
of Materials
Part 6: High Dielectric Constant (k), Gate Electrode, & Channel
Materials
SiO2 gate oxide is approaching physical limits
Thickness & Current
+V
gate
VSource
VDrain
W
M
+
poly-crystalline
Si
O
Source Contact
Insulator
S
n++ Poly Si
Gate Contact
or Electrode
Drain Contact
Insulator
SiO2 - Gate oxide
n+source - - - - - - - - - - - - - - n+drain
channel
p-Si Wafer
Crystalline Si
Cox 
t EOT 
Knowlton
L
tox
 o kox A
tox
kox
thigh  k
khigh  k
Frank, Dennard, Nowak, Soloman, Wong & Taur, Proc. IEEE Circuit & Devices , 89 (2001) 259
MSE 310/ECE 340
Electrical Properties
of Materials
M. Houssa et al., Materials Science and Engineering R, 51 (2006) 37-85
1
High Dielectric Constant (k) Materials
Bandgap versus Dielectric Constant (k)
e Hik  Ec  e Si
Trend: As k ↑, Eg ↓
Knowlton
Robertson, MRS Bulletin (March 2002) p. 217
 e Hik  e Si  Ec
Robertson, J. Vac. Sci. Technol. B, 18(3), May/Jun 2000
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MSE 310/ECE 340
Electrical Properties
of Materials
High Dielectric Constant (k) Materials
Band Offsets: High k on Si
Aspects to Consider:
1. Eg
2. Ec & Ev
3. meff
Recall in Barrier Region:
  e kx
So:
J   *  e 2 kx
2meff (V  Ee )
k

 k  meff
 meff , J 
e Hik  Ec  e Si
 e Hik  e Si  Ec
Knowlton
Robertson, MRS Bulletin (March 2002) p. 217
MSE 310/ECE 340
Electrical Properties
of Materials
J    g (k )T  k   f leftSide  E f   f rightSide  E f   dk
1 E
pˆ
& g 
where p  m g &  g 
 k
m
3
High Dielectric Constant (k) Materials
Band diagrams of MOS – compare SiO2 to high k materials
SiO2; κ~3.9
HfO2; κ~25
PbZr(0.53)Ti(0.47)O3
κ~200
Low S/C doping
Knowlton
Southwick & Knowlton, IEEE TDMR, 6(2), (2006) 136-145
4
2
MSE 310/ECE 340
Electrical Properties
of Materials
High Dielectric Constant (k) Materials
Need to consider the
Thermodynamics of the
materials system
Ellingham diagram
G –vs- Temperature
The more negative G
is, the more stable the
materials system is.
Example:
Grow Y2O3 on Si, Si will
steal oxygen from Y2O3
to form interfacial layer
(IL) of SiO2. Why?
Y 2O 3
SiO2
Al2O3
GSiO2  GY2O3
 SiO2 more stable than Y2O3
R. DeHoff, Thermodynamics of Materials, (Prentice Hall, 1996) Ch. 11, fig. 11.4
Knowlton
MSE 310/ECE 340
Electrical Properties
of Materials
5
High Dielectric Constant (k) Materials
Interfacial layer (IL) of SiO2 Present for HfO2
EOT WRT tS i O 2 & tH f O 2
TiN
3.5
3
SiO2
IL
EOT nm
HfO2
2.5
2
1.5
1
0.5
0
Crystalline
Si Channel
0
2
4
6
8
10
tH f O 2 nm 
tox ,eff  tox , physical 
Knowlton
kox
khigh  k
12
14
thigh  k
6
3
MSE 310/ECE 340
Electrical Properties
of Materials
High Dielectric Constant (k) Materials
EOT:
7 nm HfO2 & 1nm SiO2:
EOT ~ 2 nm
d 2V
d



ok
dx 2
dx
8 nm HfO2:
EOT ~ 1.25 nm
Southwick & Knowlton, IEEE TDMR, 6(2), (2006) 136-145
Knowlton
7
MSE 310/ECE 340
Electrical Properties
of Materials
High Dielectric Constant (k) Materials - NVM
Floating Gate NVM Versus SONOS (SiO2-Si3N4-SiO2-Si) NVM
SONOS Advantages over Floating Gate:
Replace poly-Si floating gate with Si3N4
Stored charge lies in defect (bound) states below Si3N4 conduction band
Improved endurance - single defect will not cause the discharge/leakage of carriers
Can reduce Thickness of TO
Si3N4 thinner than floating gate Poly Si
Carriers not “Floating” around
Minimizes interaction with neighboring memory cells
Thus, can scale down memory cell size
BL = Blocking Layer
CTL = Charge Trapping Layer
TL = Tunnel Layer
BL
CTL
TL
Knowlton
Todd Wallinger, SONOS Eases Non-Volatile Memory Integration in SoC, Semiconductor International (2007)
8
4
MSE 310/ECE 340
High Dielectric Constant (k) Materials - NVM
Electrical Properties
of Materials
BL
CTL
TL
BL
Poly
Si
CTL
TL
Floating Gate
Flat Band
Condition
BL TL
Poly
Si
Si
Si
Energy Band
Diagram
Energy Band
Diagram
Si3N4 = CTL
Gate stack scaled down in thickness & cell area
Knowlton
MSE 310/ECE 340
Electrical Properties
of Materials
Todd Wallinger, SONOS Eases Non-Volatile Memory Integration in SoC, Semiconductor International (2007)
9
High Dielectric Constant (k) Materials - NVM
Flat Band
Condition
BL
TL
Poly Si
Si
Si3N4
Energy Band
Diagram
Gate stack scaled down in thickness & cell area
Knowlton
Todd Wallinger, SONOS Eases Non-Volatile Memory Integration in SoC, Semiconductor International (2007)
10
5
MSE 310/ECE 340
Electrical Properties
of Materials
High Dielectric Constant (k) Materials - NVM
Multilayer high k dielectric films for memory applications
SONOS (poly Si–SiO –SiN–SiO –Si)
MANOS (metal–Al2O3–SiN–SiO –Si)
Sanghun et al., IEEE TED 52 (2005) 2654.pdf
TANOS (Si/SiO2/SiN/A2O3/TaN)
Lee et al., Symposium on VLSI Technology Digest of Technical Papers (2006
Knowlton
11
MSE 310/ECE 340
Electrical Properties
of Materials
Low Dielectric Constant (k) Materials
What About Low-k Dielectric Materials?
What would they be used for?
Cox 
Knowlton
 o kox A
tox
12
6
MSE 310/ECE 340
Electrical Properties
of Materials
Engineering a Memory Device – BGE & SP3
Compare and Contrast following Memory Gate Stacks:
Stack #: Metal – BL – CTL – TL -S/C
Stack 1: TiN–SiO2–Si3N4–SiO2–pSi
Stack 2: TiN–Al2O3–Ta2O5–HfO2–pSi
Stack 3: TiN–La2O3–ZnO–ZrO2–pSi
Knowlton
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
MSE 310/ECE 340
Electrical Properties
of Materials
Knowlton
13
Engineering a Memory Device – BGE & SP3
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
14
7
MSE 310/ECE 340
Electrical Properties
of Materials
Knowlton
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
MSE 310/ECE 340
Electrical Properties
of Materials
Knowlton
Engineering a Memory Device – BGE & SP3
15
Engineering a Memory Device – BGE & SP3
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
16
8
MSE 310/ECE 340
Electrical Properties
of Materials
Knowlton
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
MSE 310/ECE 340
Electrical Properties
of Materials
Knowlton
Engineering a Memory Device – BGE & SP3
17
Engineering a Memory Device – BGE & SP3
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
18
9
MSE 310/ECE 340
Electrical Properties
of Materials
Knowlton
Engineering a Memory Device – BGE & SP3
Soutwick et. al, “An Interactive Simulation Tool for Complex Multilayer Dielectric Devices”, IEEE Transactions on Device & Matls Rel., 11(2), 2011
19
MSE 310/ECE 340
Electrical Properties
of Materials
MOSFETs – Bandgap Engineering of Channel
Consider: Bandgap, mobility, effective mass,lattice matching, quantum confinement of carriers
Lattice Constants:
aSi = 5.4309 Å
aGe = 5.6577 Å
Knowlton
Cullity, Elements of X-ray Diffraction, 2nd Ed (1978) Appendix 5
From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)
20
10
MSE 310/ECE 340
Electrical Properties
of Materials
MOSFETs – Bandgap Engineering of Channel
Consider: Bandgap, mobility, effective mass, lattice
matching, quantum confinement of carriers
Lattice Constants:
aSi = 5.4309 Å
aGe = 5.6577 Å
Cullity, Elements of X-ray Diffraction, 2nd Ed (1978) Appendix 5
Knowlton IBM RJ Antoniadis et al., Continuous MOFET Performance Inc with Scaling - Strain & Channel Matl (2006)
MSE 310/ECE 340
Electrical Properties
of Materials
21
Part 5: Quantum Effects in MOS Devices
Quantization: (cont.)
2D gas in channel
SOI Gate-all-around (GAA) MOSFET:
Gate-All-Around (GAA) MOSFET is an SOI transistor in which the gate
oxide and the gate electrode are wrapped around the channel region.
Fabricated using an SOI CMOS process to which two process steps are
added
a photolithographic step
a wet etch step during which a cavity is formed under previously patterned
silicon islands.
The remarkable features of this MOSFET are that there are two channels
(at the top and the bottom of the silicon film,
The entire channel area is surrounded by good-quality gate oxide and the
gate electrode.
Knowlton
Colinge & Colinge, S/C Devices
22
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