Journal of Crystal Growth 298 (2007) 461–463
Growth of epitaxial ZnO thin film on yttria-stabilized zirconia
single-crystal substrate
Yen-Cheng Chao
a, Chih-Wei Lin
a, Dong-Jie Ke
a, Yue-Han Wu
a, Hou-Guang Chen
a,
Li Chang
a,, Yen-Teng Ho
a,b, Mei-Hui Liang
a,caDepartment of Materials Science and Engineering, National Chiao Tung University, Hsinchu 300, Taiwan bChung-Shan Institute of Science and Technology, Longtan, Taoyuan, Taiwan
cCenter of General Education, Chung-Hua University, Hsinchu 300, Taiwan
Available online 18 December 2006
Abstract
ZnO growth on yttria-stabilized zirconia (YSZ) (1 1 1) single-crystal substrate has been carried out by metalorganic chemical vapor deposition (MOCVD). High-quality epitaxial ZnO has been evidenced by X-ray diffraction (XRD) and transmission electron microscopy (TEM). Cross-sectional TEM from all deposited films reveals that the interface between ZnO and YSZ is atomically flat, and orientation relationship is deduced to be [1 1¯ 0 0]ZnO//[1 1 2¯]YSZ, [2 1¯ 1¯ 0]ZnO//[0 1 1]YSZand (0 0 0 2)ZnO//(1 1 1)YSZ. It has been found that surface
roughness increases with the substrate temperature in the range of 500–700 1C. The growth rate also varies with the temperature. r2006 Elsevier B.V. All rights reserved.
PACS: 68.55.Ac; 81.15; 68.37
Keywords: A1. Interfaces; A3. Metalorganic chemical vapor deposition; B1. Oxides; B2. Semiconducting materials
1. Introduction
Epitaxial growth of ZnO has been attracting interest as active materials in optoelectronics in recent years [1–3]. Though ZnO has been prepared by various deposition methods on a wide range of substrates, it is still a challenge for obtaining high-quality epitaxial films by chemical vapor deposition (CVD). Here, we report that it is possible to deposit high-quality ZnO films on yttria-stabilized zirconia (YSZ) (1 1 1) substrates. YSZ has the CaF2-type cubic
structure (space group Fm3m) with lattice parameter of 0.514 nm which gives about 10% lattice mismatch with ZnO. The advantages for using YSZ as substrate for CVD include the followings: relatively-low cost single-crystal wafers are commercially available; it is thermally and chemically stabilized without any reaction with ZnO at temperature below 1200 1C; and an atomically smooth
surface can be easily obtained. Epitaxial growth of ZnO on YSZ has been demonstrated by a pulsed-laser deposition technique [4]. However, there has been no report for deposition of epitaxial ZnO on YSZ by metalorganic chemical vapor deposition (MOCVD).
2. Experimental procedure
Deposition of ZnO was carried out in a vertical tube furnace at atmospheric pressure. We used zinc acetylace-tonate (Zn(C5H7O2)2) as the Zn source to benefit from its
low cost and easiness to handle[5]. The precursor of zinc acetylacetonate in solid powders was heated at 130–132 1C and N2 gas was used as carried gas. The O2 gas was
separately flowed into the furnace. The substrate tempera-ture was in the range of 450–700 1C. YSZ (1 1 1) substrate in 1 1 cm2size was cleaned by acetone before deposition. The surface roughness (rms) of as-received YSZ substrates by atomic force microscopy (AFM) is less than 0.2 nm. X-ray diffraction (XRD) and transmission electron
ARTICLE IN PRESS
www.elsevier.com/locate/jcrysgro
0022-0248/$ - see front matter r 2006 Elsevier B.V. All rights reserved. doi:10.1016/j.jcrysgro.2006.10.165
Corresponding author. Tel.: +886 3 5731615; fax: +886 3 5724727. E-mail address:[email protected] (L. Chang).
microscopy (TEM) were performed for structural char-acterization. Surface morphologies were done by AFM and scanning electron microscopy (SEM). Photoluminescence (PL) and Hall measurements were carried out for the evaluation of optical and electrical properties.
3. Results and discussion
In the XRD pattern (Fig. 1) only ZnO basal plane reflections can be seen, indicating that (0 0 0 2) planes of ZnO are parallel to the YSZ(1 1 1) surface. The grain size is estimated, using the Scherrer’s formula, to be 50 nm. The (0 0 0 2) X-ray rocking curve shows the full-width at half-maximum value of 133 arcsec, approaching the reported value of 100 arcsec for ZnO homoepitaxy by MOCVD[6]. Thus, it suggests that a high-quality ZnO film can be deposited on YSZ. There is no apparent difference among the XRD patterns from ZnO formed at different
tempera-ture in all of which ZnO shows only the (0 0 0 2) and (0 0 0 4) peaks. AFM shows that the surface roughness can be 0.7 nm for films deposited at 500 1C as seen inFig. 2(a). However, the roughness increases with the substrate temperature. For the film grown at 700 1C, SEM shows that the surface becomes rough and the grain size is increased to 160 nm. A typical electron diffraction pattern for all ZnO formation at the deposition temperature from 500–700 1C in this study is shown inFig. 3(a) and (b). The orientation relationship between ZnO and YSZ is deter-mined to be (0 0 0 2)ZnO//(1 1 1)YSZ and [1 1 2¯ 0]ZnO//
[1 1¯ 0]YSZ. From Fig. 3(a) which shows (1 1 2¯ 0)ZnO//
(2 2 0)YSZ, the in-plane mismatch can be deduced to be
about 10% as expected from the crystal lattices of ZnO and YSZ. In the cross-sectional TEM micrograph (Fig. 3(c)), a smooth ZnO film on YSZ deposited at 500 1C can be observed over the imaged region, and the film thickness is approximately 120 nm. For 600 1C deposition, TEM (not shown) shows a relative rough but thicker film. The growth rate determined from TEM is then 4 nm/s for 500 1C and 13 nm/s for 600 1C. Though the columnar structure is clearly seen in the TEM for the cases of both deposition temperatures, the SAD pattern exhibits single-crystalline characteristics. The lattice image of an interfacial region between ZnO and YSZ in [1 1¯ 0 0] is shown inFig. 4. It is readily observed that no interfacial layer exists, and the interface is quite flat. The (0 0 0 2) planes of ZnO are parallel to the (1 1 1) planes of YSZ as seen from the lattice fringes and the corresponding fast-Fourier-transform
ARTICLE IN PRESS
Intensity (a.u.) 30 40 50 60 70 80 2θ (degree) (0004) ZnO (0002) ZnO Intensity (a.u.) 0 -1000 -500 0 500 1000 Omega (arcsec)a
b
Fig. 1. (a) y–2y scan XRD pattern of ZnO deposited at 600 1C and (b) the rocking curve (o scan) for (0 0 0 2) peak.
0 0.25 0.50 0.75 1.00 μm 1.00 0.75 0.50 0.25 0 0.0 nm 10.0 nm 20.0 nm Img. Z range 12.390 nm Img. Mean -0.000000 nm Img. Raw Mean 866.42 nm Img. Rms (Rq) 0.689 nm Img. Ra 0.539 nm Img. Srf. area 1.005 μm2
Img. Srf. area diff 0.545 %
1 μm
a
b
Fig. 2. (a) AFM image of the surface of a ZnO film deposited at 500 1C and (b) SEM image of the surface deposited at 700 1C.
Y.-C. Chao et al. / Journal of Crystal Growth 298 (2007) 461–463 462
pattern shown in Fig. 4(b). The coherency across the interface is as expected from the crystal symmetry of 3 m of both oxides.
Further, we measured the film properties based on PL and Hall measurements. The PL spectrum at room temperature from ZnO deposited at 600 1C shows clearly the strong UV emission at 3.25 eV with a negligible intensity from green emission as shown in Fig. 5. For 700 1C deposition, a high intensity of green emission is excited from the ZnO film which may contain more defects. The Hall measurements give the electron mobility in the range of 20–25 cm2/V s which is observed to be independent of deposition temperature.
In summary, high-quality epitaxial ZnO films can form on YSZ(1 1 1) by atmospheric MOCVD. An atomically smooth interface with good coherency between ZnO and YSZ is observed. The surface roughness increases with deposition temperature.
Acknowledgment
This work was supported by National Science Council, Taiwan, ROC, under Contract NSC 94-2216-E-009-024.
References
[1] R. Triboulet, J. Perrie‘re, Prog. Cryst. Growth Charact. Mater. 47 (2003) 65.
[2] S.J. Pearton, D.P. Nortona, K. Ipa, Y.W. Heoa, T. Steiner, Prog. Mater. Sci. 50 (2005) 293.
[3] U¨. O¨zgu¨r, Ya.I. Alivov, C. Liu, A. Teke, M.A. Reshchikov, S. Dogan, V. Avrutin, S.-J. Cho, H. Morkoc-, J. Appl. Phys. 98 (2005) 041301. [4] K. Nomura, H. Ohta, K. Ueda, T. Kamiya, M. Orita, M. Hirano, J.
Appl. Phys. 95 (2004) 5532.
[5] Y. Kashiwaba, F. Katahira, K. Haga, T. Sekiguchi, H. Watanabe, J. Crystal Growth 221 (2000) 431.
[6] T. Gruber, C. Kirchner, A. Wagg, Phys. Stat. Sol. (b) 229 (2002) 841.
ARTICLE IN PRESS
Fig. 3. (a) and (b) SAD patterns from a cross-sectional TEM sample as shown in the bright-field image in (c) ZnO growth temperature was 500 1C.
Fig. 4. (a) HRTEM of ZnO on YSZ showing the interface and (b) the corresponding fast-Fourier-transform pattern.
0 500 1000 1500 2000 2500 3000 Y02 Y02 intensity (a.u.) wave length (nm) 400 500 600 energy (eV) 3.4 3.2 3 2.8 2.6 2.4 2.2 2
Fig. 5. PL spectrum obtained at room temperature from ZnO deposited at 600 1C.