Gallium Oxide Ramana Library/events/2013/hbcu-ucr/Gallium... · Gallium Oxide Nanostructures for...

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Gallium Oxide Nanostructures for High Temperature Sensors C.V. Ramana (PI) Evgeny Shafirovich (Co-PI) Mechanical Engineering, University of Texas at El Paso Students: Ernesto Rubio (PhD); S.K. Samala (MS) A.K. Narayana Swamy (PhD); K. Abhilash (MS) Program Manager: Richard Dunst, NETL, DOE Project: DE-FE0007225 Project Period: 10/01/2011 to 09/31/2014 1 06/12/2013 DOE UCR/HBCU Conference, June 11-13, 2013

Transcript of Gallium Oxide Ramana Library/events/2013/hbcu-ucr/Gallium... · Gallium Oxide Nanostructures for...

Gallium Oxide Nanostructures for High Temperature Sensors

C.V. Ramana (PI)Evgeny Shafirovich (Co-PI)

Mechanical Engineering, University of Texas at El PasoStudents: Ernesto Rubio (PhD); S.K. Samala (MS)A.K. Narayana Swamy (PhD); K. Abhilash (MS)

Program Manager:Richard Dunst, NETL, DOE

Project: DE-FE0007225Project Period: 10/01/2011 to 09/31/2014

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Introduction Research Objectives Experiments

► Synthesis► Characterization

Results and Discussion► Pure Ga2O3 Thin Films► W-doped Ga2O3 Thin Films

(Physical Methods) Summary & Future Work

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Energy Systems

High‐THigh‐T High‐PHigh‐P

High‐CHigh‐CHigh‐OHigh‐O

T,P ToleranceT,P Tolerance

Ox. and Cr. ResistanceOx. and Cr. Resistance

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MicrostructureMicrostructure

Choice of MaterialsChoice of Materials

SensitivitySensitivity

PoisoningPoisoning

SelectivitySelectivity

ContaminationContamination

Shelf LifeShelf Life

StabilityStability

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Fundamental Science – Phases (,,γ, and δ)

Novel Properties –Metal Doping

Surface Chemical Reactions

Chemical Sensors

Ease of Thin Film Formation 

Integration into Nano‐electronics 

Ga2O3 Wide band gap (>5 eV) semiconductor *High thermal and chemical stability (Tm: 1725 oC)*Due to a high melting point and stable structure, it is one of the most suitable materials for high temperature gas sensing.

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Tk

EPB

A

iO exp2

Activation energy

Oxygen partial pressure Boltzmann

constantTemperature

Electrical conductivity

At T>700 oC, defects equilibrium with surrounding atmosphere n type conductivity depends on oxygen partial pressure

At T< 700 oC, Ga-oxide exhibits sensitivity to reducing gases (CO, H2)

Objective 1: To fabricate high‐quality pure and dopedGa2O3‐based materials and optimize conditions to produceunique architectures and morphology at the nano scaleObjective 2: Derive the structure‐property relationships atthe nanoscale dimensions and demonstrate enhancedhigh‐temperature oxygen sensing and stabilityObjective 3: To promote research and education in thearea of sensors and controls

Goal: Design the high temperature oxygen sensors(employing Ga2O3‐based nanostructures)

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Target (for Deposition)Ga2O3 & W

Substrate(s): Si(100) Alumina

MaterialsGa-oxide

Cu-backing plate

2 inch.

1/8 inch.

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RF magnetron sputtering Deposition Conditions

Fixed:- Base pressure ~10-6 Torr- Powers: Ga2O3100 W- Target-Substrate distance: 7 cm- Sputtering gas: Argon + O2

Variables: Sample set 1 (Intrinsic): Substrate Temperature: RT-500 ˚CSample set 2 (W-Doped): Tungsten Target Power (50 to 100W)Substrate Temperature = 500 ˚C

Fabrication – Thin Films

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Sample set 3 (W-Doped): Target Powers = const.; Substrate temperature varied from 500 to 800˚C

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Characterization

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Characterization (cont.)

High Temperature Furnace for annealing process

UV-vis-Spectrophotometry

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PVD: Sputtering

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10 20 30 40 50 60 70 80 90

Si (2

00)

Si (2

00)

800C

(020

)(

221)

(020

)(

221)

500C

400C

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Crystal Structure

300 400 500 600 70010

15

20

25

30

35 Exponential Fit

Gra

in S

ize

(nm

)

Temperature (C)

L = Lo exp (-∆E/kBT)L: Average size L0: Pre-exp. factor (film, substrate materials) ∆E: Activation energy, kB: Boltzmann constant and T: Absolute temperature.

500 °C is favorable to provide sufficient energy for Ga2O3film crystallization (β-phase)

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Morphology

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Composition - RBS

200 400 600 8000

400

800

1200

1600

2000

2400

2800

400 800 1200 1600

2 MeV He+ Ga2O3//Si(100)Ts - 600 C

Energy (KeV)

Channel Number

Bac

ksca

ttere

d Io

n Yi

eld

(Cou

nts)

experimental simulated

OGa

Si

200 400 600 8000

400

800

1200

1600

2000

2400

2800

400 800 1200 1600Energy (KeV)

2 MeV He+ Ga2O3 //Si(100)Ts - 500C

Bac

ksca

ttere

d Io

n Yi

eld

(Cou

nts)

Channel Number

experimental simulated

OSi

Ga

200 400 600 8000

400

800

1200

1600

2000

2400

2800

400 800 1200 1600

Channel Number

Bac

ksca

ttere

d Io

n Yi

eld

(Cou

nts)

2 MeV He+ Ga2O3 //Si(100)Ts - 300 C

experimental simulated

Energy (KeV)

O SiGa

200 400 600 8000

400

800

1200

1600

2000

2400

2800

400 800 1200 1600

2 MeV He+ Ga2O3 //Si(100)

Ts - RT

Channel Number

Energy (KeV)

Bac

ksca

ttere

d Io

n Yi

eld

(Cou

nts)

experimental simulated

O

Si

Ga

0 100 200 300 400 500 600 700 800 900

1.2

1.5

1.8

O/G

a

Temperature (C)

O/Ga

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Composition - XPS

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Ga 2p peak

As Grown Sputtered

Chemical Shift in Ga 2p BE – ~1118 eV; ~1145 eVOriginal Ga 2p BE – 1117eV; 1144 eV (represented by blue lines)

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Microstructure – Phase Diagram 

100 200 300 400 500 600 700 800

Slightly excess oxygen

Stoichiometric T

rans

ition

Tem

pera

ture

B

egin

ing

of N

anoc

ryst

allin

e Fi

lms

Grain size 10- 40 nm

-phase

Ga2O3 Films

Amorphous

Substrate Temperature (C)

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200 300 400 500 600 700 800

20

40

60

80

100

120

Tran

smitt

ance

, % T

Wavelength (nm)

RT 200 C 300 C 500C 600C 800C

0 100 200 300 400 500 600 700 800 9004.90

4.95

5.00

5.05

5.10

5.15

5.20

Ban

dgap

(eV)

Temperature (C)

Electronic Properties

(αhν) = B (hν-Eg)1/2

hν: energy of the incident photon, α: absorption coefficient, B: absorption edge width parameter, Eg:band gap.

α = [1/t]ln[T/(1-R)2]T: transmittance R: reflectance t : film thickness

PVD: Sputtering

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200 ̊C

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300 ̊C

Chemical Composition (RBS)

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W‐Doped filmsW‐Power (Watts)

W‐Content (Atomic %)

Thick‐ness

0 0 38 nm

50 8.35 32 nm

75 9.58 42 nm

100 12.5 51 nm

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Crystal Structure – Power dependence

Only Gallium oxide phase is present

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No secondary phase formation

Morphology (Power Dependent)

Pure Gallium Oxide Films show grains throughout the surface, and W-doped films

Pure Gallium Oxide Films show grains throughout the surface, and W-doped films avoid crystallites complete growth

Ts=500°C

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Optical Propertiestdep= 30min

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Band Gap (Power dependence)

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Reduction by ~0.75-1.00 eV with the inclusion of tungsten into Ga-oxide films!

E.J. Rubio and C.V. Ramana, Appl. Phys. Lett. 102, 191913 (2013).

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Crystal Structure – (after annealing)

Deposition Temperature Ts=500 °C;Annealing TemperatureTa=700 °C for 30 min

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Crystal Structure – (Temp. Dependent)

Only β-phase presented for all films.

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Morphology – Broad View

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Why does it work?

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Crystallography: MonoclinicIonic Size:

Comparable (W6+ vs. Ga3+)

Electronegative Values:Similar

W Ga

Morphology – Broad View

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ImpactJournal Publications:1. E.J. Rubio and C.V. Ramana, Appl. Phys.

Lett. 102, 191913 (2013).2. A.K. Narayana Swamy, E. Shafirovich, and

C.V. Ramana, Ceram. Inter. 39, 7223 (2013).3. S.K. Samala, E.J. Rubio, M. Noor-A-Alam,

G. Martinez, S. Manandhar, V. Shutthanandan, S. Thevuthasan, and C.V. Ramana, J. Phys. Chem. C 117, 4194 (2013).

4. Two others (under preparation)

Conference Presentations:1. International Materials Research Congress (IMRC) – to be

presented 2. International Conference on Metallurgical Coatings and Thin

Films, April 29 – May 3, 2013, San Diego, CA3. AVS International Symposium, October 28 – November 2, 2012

Tampa, FL4. Southwest Energy Symposium, March 24, 2012, El Paso, TX

Education & Training:1. Ernesto J. Rubio: PhD

(Full)2. A.K. Narayana Swamy:

PhD (part of disseration)3. Sampath K. Samala: MS

(thesis)4. Abhilash Kongu: MS

(non-thesis)

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Future Work

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Materials Fabrication(Pure Ga‐Oxide) Materials 

Character.& W‐Doping

Testing and Performance Evaluation

Y-1

Y-2

Y-3

Future Work

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Future Work

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Detailed Electrical and Sensor Characteristics (UTEP)

SUNY – Michael Carpenter (Plasmonics)

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Summary & Conclusions

Pure and W-doped Ga‐oxide thin films were grownand characterized

Experimental conditions were optimized to obtainGa‐oxide materials with wide controlled structureand morphology in a wide range

Stability of β‐phase with controlled electronicproperties is demonstrated (with W‐incorporation)

Preliminary results obtained on the electricalproperties are encouraging

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AcknowledgementsDOE‐NETLRichard DunstEMSL/PNNL, Richland, WA

10/25/2011 UTSR Workshop, Oct. 25-27, 201106/12/2013 DOE UCR/HBCU Conference, June 11-13, 2013

THANK YOU!