technology thin films zno:al were prepared by rf diode sputtering from zno + 2wt % al 2 o 3 target....

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Technology Thin films ZnO:Al were prepared by RF diode sputtering from ZnO + 2wt % Al 2 O 3 target. It is a plasma assisted deposition method which involves a significant energetic bombardment of neutral atoms, ions and electrons on the growing film. RF power and substrate temperature are determining for the properties of sputtered ZnO films [ 3 ]. 38 40 42 0 100 200 300 400 500 600 800 W 600 W 400 W In ten s ity (c p s ) 2 (degrees) 200 W 40 42 0 500 1000 1500 2000 2500 300 °C RT 100 °C 200 °C 300 °C In te n s ity (c p s ) 2 (degrees) -110 -100 -90 -80 -70 0 2000 6000 8000 300 °C 200 °C 100 °C RT In ten sity (cp s) (degrees) 300°C (002) (101) RT (002) 100°C (002) 200°C (002) K. Shtereva 1) , S. Flickyngerová 2) , P. Šutta 3) , M. Netrvalová 3) , I. Novotný 2) and V. Tvarožek 2) 1) Department of Electronics, University of Rousse, Studentska 8, 7017 Rousse, Bulgaria 2) Department of Microelectronics, Slovak University of Technology, Ilkovicova 3, 812 19 Bratislava, Slovakia 3) West Bohemian University, New technologies – Research Centre, Univerzitni 8, 306 14 Plzen, Czech Republic Transparent and conductive ZnO:Al Transparent and conductive ZnO:Al prepared by RF diode sputtering prepared by RF diode sputtering Introduction The unique material properties in combination with a great natural abundance and low cost, make zinc oxide a promising transparent conducting oxide (TCO) for application in thin film solar cells and various optoelectronic devices [1, 2]. In addition it is an environment friendly material. A matter of great importance for these industrial applications is the availability of a cost effective deposition technology. RF sputtering is such method that offers a deposition at low temperatures, safety advantages, and where the use of the toxic gases is avoided. Structure characterization XRD patterns show polycrystalline ZnO:Al thin films with a strong texture in the [001] direction perpendicular to the substrate 2-dimensional XRD patterns display elliptic diffraction spots of identically orientated polycrystals The widths of azimuthal (002) line profiles (FWHM of the -scan ) decrease from 15 to 3.5° with increasing energy delivered to the growing film during the deposition The up shift of the 2 with increasing RF powers and temperatures is a result of the increase of Al 3+ substituents (Al 3+ that substitute for Zn 2+ in the ZnO lattice) and a reduction of the interplanar distance, which changes the lattice distortion in ZnO:Al films from compressive to tensile lattice stresses Asymmetry of the (002) diffraction line indicates a region with heterogeneous structure at the substrate – film interface for films grown at room substrate temperature, and completely diminished at higher substrate temperatures The RF power and temperature growth, result in the larger grains (growth from 60 to more than 200 nm) and better crystalline structure (no line asymmetry) 200 400 600 800 1000 1200 10 -3 10 -2 10 -1 2 4 6 8 0.5 1.0 1.5 2.0 C o n c e n tratio n n [1 0 20 cm -3 ] R e sis tiv ity [ cm ] R F pow er P [W ] M ob ility H [c m 2 / V s] H n 0 100 200 300 10 -3 10 -2 3 6 9 12 1.0 1.5 2.0 2.5 C o n ce n tratio n n [1 0 20 cm -3 ] R e s istiv ity [ cm ] S u b strate tem p eratu re T s [°C ] M ob ility H [cm 2 / V s] H n -100 0 100 200 300 10 -3 10 -2 300°C 200°C 100°C S ubstrate temperature RT R e sis tiv ity [ cm ] H allm easurem en t T [°C ] Electrical properties Minimum resistivity 2.6 x 10 -3 cm, as a result of the highest carrier concentration 2 x 10 20 cm -3 and mobility 7.81 cm 2 /Vs, is obtained for ZnO:Al grown at 1200 W RF power and RT The carrier concentration goes straightforwardly up (to 2.4 x 10 20 cm -3 ) with increasing temperatures, as a result of the increased Al 3+ substituents into the films ZnO:Al thin films deposited with 800W and 200ºC exhibit strong degenerated semiconductor behaviour, the resistivity rises with the temperature at temperature-dependent Hall measurements 300 400 500 900 1000 0 20 40 60 80 100 C o rn in g g lass 1200 W 1000 W 800 W 600 W 400 W 200 W T ra n sm itta n c e [% ] Wavelength [nm ] Optical properties The average transmittance of ZnO:Al thin films, including Corning glass substrate, varies from 82 ÷ 86 % with increasing RF power The sharp absorption edge appears at ~ 380 nm wavelength and the enlargement of the sputter power causes the blue shift of the cut – off wavelength Optical bandgap Eg (~3.3 eV) widens with increasing RF power and temperature 1 µm The surface images of ZnO:Al prepared with 800 W RF power and 200ºC substrate temperature obtained by means of SEM and AFM show a nanostructured surface References [1]Yoo J, Lee J, Kim S, Yoon K, Park I J, Dhunge S K, Karunagaran B, Mangalaraj D and Yi J 2005 Thin Solid Films 480– 481 213– 217 [2]Hüpkes J, Rech B, Calnan S, Kluth O, Zastrow U, Siekmann H and Wuttig M 2006 Thin Solid Films 502 286 – 291 [3]Tvarozek V, Novotny I, Sutta P, Flickyngerova S, Schtereva K and Vavrinsky E 2007 Thin Solid Films doi:10.1016/j.tsf.2007.03.125 (in press) Conclusions The properties of ZnO:Al thin films were considerable modified by RF power and substrate temperature. The RF diode sputtering method can partially replace an influence of substrate temperature on growing film by the increasing of RF power, which becomes greater in the bombardment of substrate by energetic secondary electrons and ions. The lowest resistivity (2 x 10 -3 cm) and the highest mobility (12 cm 2 /Vs), carrier concentration (2 x 10 20 cm -3 ) and transmittance ( > 82% including the substrate) are obtained in highly textured ZnO:Al films (widths of azimuthal line profiles (002) has a minimum FWHM ~3.26º) prepared at high RF power (800 W) and substrate temperature (200°C). Motivation Development: high transparent and conductive ZnO:Al thin films for solar cells and optoelectronic devices application Investigate correlations: structure surface morphology electrical parameters optical parameters STRUCTURE Surface morphology Opti cal pa ramet ers Electrical parameter s

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Page 1: Technology Thin films ZnO:Al were prepared by RF diode sputtering from ZnO + 2wt % Al 2 O 3 target. It is a plasma assisted deposition method which involves

Technology Thin films ZnO:Al were prepared by RF

diode sputtering from ZnO + 2wt % Al2O3 target.

It is a plasma assisted deposition method which involves a significant energetic bombardment of neutral atoms, ions and electrons on the growing film. RF power and substrate temperature are determining for the properties of sputtered ZnO films [ 3 ].

38 40 420

100

200

300

400

500

600

800 W

600 W400 W

Inte

ns

ity

(c

ps

)

2 (degrees)

200 W

40 420

500

1000

1500

2000

2500

300 °C

RT

100 °C

200 °C

300 °C

Inte

ns

ity

(c

ps

)

2 (degrees)

-110 -100 -90 -80 -700

2000

6000

8000

300 °C

200 °C

100 °C

RT

Inte

nsi

ty (

cps)

(degrees)

300°C

(002) (101)

RT

(002)

100°C

(002)

200°C

(002)

K. Shtereva1), S. Flickyngerová2), P. Šutta3), M. Netrvalová3), I. Novotný2) and V. Tvarožek2)

1) Department of Electronics, University of Rousse, Studentska 8, 7017 Rousse, Bulgaria2) Department of Microelectronics, Slovak University of Technology, Ilkovicova 3, 812 19 Bratislava, Slovakia3) West Bohemian University, New technologies – Research Centre, Univerzitni 8, 306 14 Plzen, Czech Republic

Transparent and conductive ZnO:Al Transparent and conductive ZnO:Al prepared by RF diode sputteringprepared by RF diode sputtering

IntroductionThe unique material properties in combination with a great natural abundance and low cost, make zinc oxide a promising transparent conducting oxide (TCO) for application in thin film solar cells and various optoelectronic devices [1, 2]. In addition it is an environment friendly material.

A matter of great importance for these industrial applications is the availability of a cost effective deposition technology. RF sputtering is such method that offers a deposition at low temperatures, safety advantages, and where the use of the toxic gases is avoided.

Structure characterizationXRD patterns show polycrystalline ZnO:Al thin films with a strong texture in the [001] direction perpendicular to the substrate

2-dimensional XRD patterns display elliptic diffraction spots of identically orientated polycrystals

The widths of azimuthal (002) line profiles (FWHM of the -scan ) decrease from 15 to 3.5° with increasing energy delivered to the growing film during the deposition

The up shift of the 2 with increasing RF powers and temperatures is a result of the increase of Al3+ substituents (Al3+ that substitute for Zn2+ in the ZnO lattice) and a reduction of the interplanar distance, which changes the lattice distortion in ZnO:Al films from compressive to tensile lattice stresses

Asymmetry of the (002) diffraction line indicates a region with heterogeneous structure at the substrate – film interface for films grown at room substrate temperature, and completely diminished at higher substrate temperatures

The RF power and temperature growth, result in the larger grains (growth from 60 to more than 200 nm) and better crystalline structure (no line asymmetry)

200 400 600 800 1000 120010-3

10-2

10-1

2

4

6

8

0.5

1.0

1.5

2.0

Co

nce

ntr

atio

n n

[10

20cm

-3]

Res

isti

vity

[

cm]

RF power P [W]

Mo

bil

ity H

[cm

2 / V

s]

H

n

0 100 200 30010-3

10-2

3

6

9

12

1.0

1.5

2.0

2.5

Co

nce

ntr

atio

n n

[10

20cm

-3]

Res

isti

vity

[

cm]

Substrate temperature Ts [°C]

Mo

bil

ity H

[cm

2 / V

s]

H

n

-100 0 100 200 30010-3

10-2

300°C

200°C

100°C

Substrate temperatureRT

Res

isti

vity

[

cm]

Hall measurement T [°C]

Electrical properties Minimum resistivity 2.6 x 10-3 cm, as a result of the highest carrier concentration 2 x 1020 cm-3 and mobility 7.81 cm2/Vs,

is obtained for ZnO:Al grown at 1200 W RF power and RT

The carrier concentration goes straightforwardly up (to 2.4 x 1020 cm-3) with increasing temperatures, as a result of the increased Al3+ substituents into the films

ZnO:Al thin films deposited with 800W and 200ºC exhibit strong degenerated semiconductor behaviour, the resistivity rises with the temperature at temperature-dependent Hall measurements

300 400 500 900 10000

20

40

60

80

100Corning glass

1200 W

1000 W

800 W

600 W

400 W

200 W

Tra

ns

mit

tan

ce

[%

]Wavelength [nm]

Optical properties The average transmittance of ZnO:Al thin films, including

Corning glass substrate, varies from 82 ÷ 86 % with increasing RF power

The sharp absorption edge appears at ~ 380 nm wavelength and the enlargement of the sputter power causes the blue shift of the cut – off wavelength

Optical bandgap Eg (~3.3 eV) widens with increasing RF power and temperature

1 µm

The surface images of ZnO:Al prepared with 800 W RF power and 200ºC substrate temperature obtained by means of SEM and AFM show a nanostructured surface

References

[1] Yoo J, Lee J, Kim S, Yoon K, Park I J, Dhunge S K, Karunagaran B, Mangalaraj D and Yi J 2005 Thin Solid Films 480–481 213– 217

[2] Hüpkes J, Rech B, Calnan S, Kluth O, Zastrow U, Siekmann H and Wuttig M 2006 Thin Solid Films 502 286 – 291

[3] Tvarozek V, Novotny I, Sutta P, Flickyngerova S, Schtereva K and Vavrinsky E 2007 Thin Solid Films doi:10.1016/j.tsf.2007.03.125 (in press)

Conclusions The properties of ZnO:Al thin films were considerable

modified by RF power and substrate temperature. The RF diode sputtering method can partially replace an influence of substrate temperature on growing film by the increasing of RF power, which becomes greater in the bombardment of substrate by energetic secondary electrons and ions.

The lowest resistivity (2 x 10-3 cm) and the highest mobility (12 cm2/Vs), carrier concentration (2 x 1020 cm-3) and transmittance ( > 82% including the substrate) are obtained in highly textured ZnO:Al films (widths of azimuthal line profiles (002) has a minimum FWHM ~3.26º) prepared at high RF power (800 W) and substrate temperature (200°C).

MotivationDevelopment:

high transparent and conductive ZnO:Al thin films for solar cells and optoelectronic devices application

Investigate correlations:

structure surface morphology electrical parameters optical parameters

STRUCTURE

Surface morphology

Optical

parameters

Elect

rical

param

eter

s