Measurements of the E-field Breakdown and Band Offsets of SiO 2 on GaN
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Transcript of Measurements of the E-field Breakdown and Band Offsets of SiO 2 on GaN
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
NC STATE UNIVERSITY UCSB
Measurements of the E-field Breakdown and Band Offsets of
SiO2 on GaN
Ted Cook, Ed Hurt, Kieran Tracy, R.F. Davis, G. Lucovsky,
and R.J. Nemanich
North Carolina State University
Raleigh, NC 27695-8202 USA
February 12, 2002
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Introduction
• The band offsets have a direct effect on the properties of the interface, and therefore affect the reliability and stability of the device
• Investigation of the band offsets, as well as their effects, such as E-field breakdown, is important for device fabrication, and will be explored in this study
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Goal and Motivation
Goal:• Measure the Valence Band Offsets between
atomically clean GaN and SiO2 using photoemission techniques
Motivation:• Passivation of high voltage devices• Wafer Bonding – fusion bonded interfaces• Gate insulator applications
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Experimental Procedure
1. Achieve atomically clean GaN surface using CVC anneal in NH3 atmosphere @ 860°C for 15 minutes
2. XPS and UPS performed after each of the following steps to track the evolution of peak shifts
1. Deposition of 2Å Si via MBE
2. Deposition of a second 2Å Si layer
3. Oxidation of Si layer using a Remote O2 plasma
4. Deposition of 2Å, and oxidation of the Si layer
5. 650°C anneal for 15 minutes to densify the oxide
6. Deposition of 3Å, and oxidation of the Silicon layer
7. Final anneal at 650°C for densification
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Integrated UHV Surface and Interface Processing System
CVD Diamond
High Voltage Testing
Field Emission XPS GSMBE
AES / LEEDe-beam evap
Si-GeMBE
ARUPS
Hydrogen/OxygenPlasma
LoadLock
ECR N2
PlasmaWafer
Bonding
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Proposed Valence Band Line-up between n-GaN and SiO2
-6.0
-5.5
-5.0
-4.5
-4.0
-3.5
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0 Ef
Ec
Ev
Evac
Eg = 3.40eV Ef-Ev = 3.32eV
= 2.9eV
Eg = 9.0eV
Ef-Ev = 5.30eV
Ec-Ef =0.08eV
Ec-Ef = 3.70eV
= 1.1eV
Ec = 3.6eV
Ev = 2.0eV
GaN SiO2Clean
Ed = 0.3eV
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Gallium 3d XPS Evolution of n-type GaN
1012141618202224262830
Binding Energy (eV)
Inte
nsi
ty (
au)
CVC
Final Anneal 650°C
2Å Si Total
4Å Si Total
O Plasma
6Å Si Total & O Plasma
Anneal 650°C
9Å Si Total & O Plasma
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Energy Band Diagram
Clean GaN Surface Final Surface
Ef Ef
CB CB
VBVB
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UPS Spectra of VB turn-on
-10 -9 -8 -7 -6 -5 -4 -3 -2 -1 0Fermi Level Referenced Energy (eV)
Co
un
ts (
a.u
.)
CVC GaN
650°C Final Anneal
0.3 eV shift due to band bending
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Valence Band Offset between GaN and SiO2
-6.0
-5.5
-5.0
-4.5
-4.0
-3.5
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0 Ef
Ec
Ev
Evac
Eg = 3.40eV Ef-Ev = 3.32eV
= 2.9eV
Eg = 9.0eV
Ef-Ev = 5.30eV
Ec-Ef =0.08eV
Ec-Ef = 3.70eV
= 1.1eV
Ec = 3.6eV
Ev = 2.0eV
GaN SiO2Clean
Ed = 0.3eV
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Oxygen 1s XPS Spectra showing Oxide Formation
520522524526528530532534536538540Binding Energy (eV)
Inte
ns
ity
(a
u)
CVC
Final Anneal 650°C
2Å Si Total
4Å Si Total
O Plasma
6Å Si & O Plasma
Anneal 650°C
9Å Si & O Plasma
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UPS Spectra of Spectral Width
-21 -20 -19 -18 -17 -16 -15 -14 -13 -12 -11 -10 -9 -8 -7 -6 -5 -4 -3 -2 -1 0
Fermi Level Referenced Energy (eV)
Co
un
ts (
a.u
.)
CVC GaN
650°C Final Anneal
W=11.1 eVEg SiO2 =9.0 eV
Eg GaN =3.4 eVW=14.9 eV
=21.2-11.1-9.0 = 1.1 eV
=21.2-14.9-3.4 = 2.9 eV
=h-W-Eg
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Electron Affinity difference between GaN and SiO2
-6.0
-5.5
-5.0
-4.5
-4.0
-3.5
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0 Ef
Ec
Ev
Evac
Eg = 3.40eV Ef-Ev = 3.32eV
= 2.9eV
Eg = 9.0eV
Ef-Ev = 5.30eV
Ec-Ef =0.08eV
Ec-Ef = 3.70eV
= 1.1eV
Ec = 3.6eV
Ev = 2.0eV
GaN SiO2Clean
Ed = 0.3eV
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Models of Heterojunctions
• Electron Affinity Model
Valid if small or no change in the interface Dipole• Interface Dipole Model
Change in the Electric field at interface• Deviation from the electron affinity of the heterojunction
alignment represents the interface dipole
EAM IDM
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Interface Dipole in Band Line-up of GaN and SiO2
=1.9 eV
-6.0
-5.5
-5.0
-4.5
-4.0
-3.5
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0 Ef
Ec
Ev
Evac
Eg = 3.40eV Ef-Ev = 3.32eV
= 2.9eV
Eg = 9.0eV
Ef-Ev = 5.30eV
Ec-Ef =0.08eV
Ec-Ef = 3.70eV
= 1.1eV
Ec = 3.6eV
Ev = 2.0eV
GaN SiO2Clean
Ed = 0.3eV
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Conclusions for n-type experiment
• Special care has been taken to prevent oxidation of gallium
• Band bending of ~0.3 eV for CVC GaN surface• Electron Affinity ~2.9 eV for CVC GaN surface
• Flat Bands at the GaN-SiO2 Interface
• Valence Band Offset of ~2 eV for GaN-SiO2 for 1x1017
cm-3 n-type GaN
• Conduction Band offset of ~3.6 eV for GaN-SiO2 assuming EgSiO2 =9.0 eV
• Deviation from the Electron Affinity model due to Interface dipole of ~1.9 eV
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Gallium 3d XPS Evolution of p-type GaN
1012141618202224262830
Binding Energy (eV)
Inte
ns
ity
(a.u
.)
Clean GaN
2Å Si
4Å Si
4Å Si and O2 Plasma
6Å Si and O2 Plasma
650 C anneal
9Å Si and O2 Plasma
Final anneal
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Proposed Valence Band Line-up between p-GaN and SiO2
-6.0
-5.5
-5.0
-4.5
-4.0
-3.5
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0 Ef
Ec
Ev
Evac
Eg
= 3.40eV
Ef-Ev = 2.2eV
Eg = 9.0eVEf-Ev = 4.5eV
Ec-Ef =3.1eV
Ec-Ef = 4.5eV
Ec = 3.3eV
Ev = 2.3eV
GaN SiO2
EB=0.3eV
Ef-Ev=1.7eV
Clean
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Conclusions for p-type experiment
• Initial Band Bending of 1.4 eV for CVC GaN surface• Additional downward Band Bending of ~0.5 eV as
the surface was formed
• Valence Band offset of ~2.3 eV for GaN-SiO2 for 2x1018 cm-3 p-type GaN
• Conduction Band Offset of 3.3 eV for GaN-SiO2 assuming Eg Sio2 =9.0 eV
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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E-field Breakdown Procedure
1. Achieve atomically clean GaN surface using CVC anneal in NH3 atmosphere @ 860°C for 15 minutes
2. Deposit 4Å Si via MBE on surface to help prevent oxidation of the Gallium
3. Deposit 300Å SiO2 via Remote O2 Plasma
4. Anneal to 650°C to densify the oxide
5. Form 0.068 mm2 Al contacts on the surface using photolithographic techniques
6. Electrical characterization of sample
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Device Structure for Electrical Testing
SiC
SiO2GaN AlN
W Contact
Al Contacts V
CRT
I
v
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Breakdown Frequency
0
2
4
6
8
10
12
1 6 11 16 21 26 31 36 41 46 51 56 61 66 71 76 81 86 91 96 101 106
Voltage
Co
un
ts
300Å SiO2
unintentionally doped, n-type <1.0x1017 cm-3
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Conclusions
• These high values of breakdown voltage lends to the notion that the GaN layer is having an insulating effect
• A full understanding of this effect requires more study
• Film deposition rate of 2.5 Å/min established; verified by ellipsometry and C-V measurements
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors
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Future Work
• Reduce Band Bending for p-type GaN/SiO2
-Improve cleaning methods
-Oxide integrity
• Effect of different passivation layers
– Si3N4
– High k dielectrics