Measurements of the E-field Breakdown and Band Offsets of SiO 2 on GaN

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Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap NC STATE UNIVERSITY UCSB Measurements of the E-field Breakdown and Band Offsets of SiO 2 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

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Measurements of the E-field Breakdown and Band Offsets of SiO 2 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. Introduction. - PowerPoint PPT Presentation

Transcript of Measurements of the E-field Breakdown and Band Offsets of SiO 2 on GaN

Page 1: 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

Page 2: 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

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

Page 3: 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

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

Page 4: 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

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

Page 5: 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

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

Page 6: 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

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

Page 7: 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

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

Page 8: 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

Energy Band Diagram

Clean GaN Surface Final Surface

Ef Ef

CB CB

VBVB

Page 9: 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

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

Page 10: 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

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

Page 11: 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

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

Page 12: 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

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

Page 13: 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

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

Page 14: 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

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

Page 15: 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

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

Page 16: 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

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

Page 17: 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

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

Page 18: 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

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

Page 19: 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

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

Page 20: 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

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

Page 21: 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

Device Structure for Electrical Testing

SiC

SiO2GaN AlN

W Contact

Al Contacts V

CRT

I

v

Page 22: 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

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

Page 23: 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

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

Page 24: 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

Future Work

• Reduce Band Bending for p-type GaN/SiO2

-Improve cleaning methods

-Oxide integrity

• Effect of different passivation layers

– Si3N4

– High k dielectrics