Journal of Nanotechnology

Journal of Nanotechnology / 2009 / Article

Research Letter | Open Access

Volume 2009 |Article ID 280797 |

J. C. Johnson, S. P. Ahrenkiel, P. Dutta, V. R. Bommisetty, "Nucleation and Growth of Crystalline Grains in RF-Sputtered TiO2 Films", Journal of Nanotechnology, vol. 2009, Article ID 280797, 4 pages, 2009.

Nucleation and Growth of Crystalline Grains in RF-Sputtered TiO2 Films

Academic Editor: Xiaowei Sun
Received03 Jun 2009
Accepted25 Jul 2009
Published12 Oct 2009


Amorphous TiO2 thin films were radio frequency sputtered onto siliconmonoxide and carbon support films on molybdenum transmission electron microscope (TEM) grids and observed during in situ annealing in a TEM heating stage at 250C. The evolution of crystallization is consistent with a classical model of homogeneous nucleation and isotropic grain growth. The two-dimensional grain morphology of the TEM foil allowed straightforward recognition of amorphous and crystallized regions of the films, for measurement of crystalline volume fraction and grain number density. By assuming that the kinetic parameters remain constant beyond the onset of crystallization, the final average grain size was computed, using an analytical extrapolation to the fully crystallized state. Electron diffraction reveals a predominance of the anatase crystallographic phase.

1. Introduction

The broad range of industrial and technological applications for the wide-gap semiconductor TiO2 has grown to include numerous roles in energy conversion and storage, particularly relating to photovoltaics [1] and photocatalysis [2]. Along with its useful electrical and optical properties [3], TiO2 provides the benefits of low toxicity, good chemical stability, and ease of fabrication [4]. As-deposited, amorphous-titania thin films are commonly produced at low temperature by a range of methods, commonly spincoating of sol-gel precursors [5] and physical vapor deposition [6]. Postdeposition crystallization provides additional influence on crystallographic phase and the promotion of desirable microstructural characteristics, with potential relevance toward developing new, low-cost methods of synthesis, while also permitting fundamental studies of materials properties.

Under ambient conditions, kinetic barriers typically prevent the rapid phase transformation from a metastable, amorphous microstructure to a crystallized, solid state [7]. Mechanisms leading to crystallization may include spontaneous grain nucleation and grain growth, which can be thermally activated at elevated temperatures, using thermal annealing [8, 9] or electron-beam irradiation [1012]. This work aims to shed light on the kinetics of nucleation and growth crystalline grains in as-deposited amorphous, RF-sputtered TiO2 films, during isothermal annealing in a TEM heating stage. Several experiments have examined crystallization during thermal annealing of sol-gel TiO2 films [8, 9, 1214], which may be driven by the coalescence of nanosized amorphous nuclei. Metallurgical phase transformations are more often associated with growth of individual grains into the surrounding amorphous matrix [15], leading to a poly- or microcrystalline grain structure. The data presented here are analyzed from the perspective of classical phase-transformation theory, assuming homogenous nucleation and isotropic grain growth. The final, average grain size in these films is predicted by analytical extrapolation of the modeled behavior to the fully crystallized state. The goal is to understand and influence the crystallization process, providing for optimization of material quality and improvements in the performance of TiO2 films for device applications.

2. Experiment

TiO2 was radio-frequency sputtered onto silicon-monoxide coated and carboncoated, 200-mesh Mo TEM grids, obtained from Electron Microscopy Sciences. A steel TEM grid holder was used to suspend the grids in the reactor in an inverted orientation, with contact only to the grid periphery. The thickness of the support films is specified by the manufacturer to be in the range of 15–30 nm for silicon monoxide and 20–30 nm for carbon. A 2-diameter TiO2 target with 99.9% purity from Kurt J. Lesker Company was sputtered with a process pressure of 5 mTorr, plasma power of 150 W, deposition rate of 0.02 nm/s, Ar gas flow rate of 20 sccm, and a nominal thickness of =100nm. To reduce crystallization during deposition, no substrate heating was used. However, we note the presence, prior to postdeposition treatment, of small crystalline nuclei, representing less than 1% of the total sample volume.

The samples were imaged on a Hitachi H7000-FA TEM, operated at 125 KV, using an Olympus SIS Veleta 14-bit, 4-megapixel CCD side-mount camera. The Olympus SIS iTEM imaging software was used to acquire the image series, by automated acquisition at 2-second intervals. In situ annealing was accomplished with a Gatan Model 628 single-tilt heating holder. The heating stage uses a tantalum furnace, capable of temperatures over 1000C, with a hex-ring retaining screw to secure the sample. To reach a final dwell temperature of 250C, the heating stage was ramped up initially to 100C, then 200C, and allowed to dwell at each temperature for approximately 1–2 minutes to reduce drift. Enhanced crystallization in the analyzed region was sometimes observed, presumably due to local heating by the electron beam. TEM image series were taken in conical dark-field mode, using beam precession about the optic axis at 20 Hz, with an objective aperture of diameter 3.3 nm1 placed in the back focal plane of the objective lens to increase contrast between amorphous and crystalline regions. The beam tilt was adjusted so that the anticipated position of the first strong diffraction ring was approximately centered on the optic axis.

A subset of images acquired 20 seconds apart was selected for quantitative analysis. Using Adobe Photoshop Elements 2.0, a portion of each image was cropped from a common area. Automatic and manual edge recognition tools were used to differentiate crystalline from amorphous regions. The segmented images were then imported to Gatan Digital Micrograph to determine the crystalline volume fraction 𝑋𝑐=𝑉𝑐/𝑉, where 𝑉𝑐 and 𝑉 are the crystallized and total volumes, respectively, which were assumed to be proportional to the projected areas. Direct grain counting was performed using an elliptical annotation tool to demarcate previously counted grains, to determine the areal grain number density 𝜌𝑔=𝑁𝑔/𝐴, where 𝑁𝑔 is the number of grains in the film area 𝐴. Errors in 𝑋𝑐 were taken as 4𝑋𝑐(1𝑋𝑐)(5%), where 5% was estimated to be the maximum random error in repeated measurements of 𝑋𝑐. The fractional error in 𝜌𝑔 was taken as 𝑁𝑔1/2.

For cinematic visualization of the entire crystallization process, the contrast for all the photos was normalized, then the entire image series was aligned by a combination of cross-correlation and iterative difference minimization about areas containing clearly identifiable features. The image series was then imported to Apple QuickTime to generate a video representation.

Selected-area electron diffraction patterns were acquired from circular areas several microns in diameter. Line patterns were then generated by rotational averaging in Digital Micrograph, allowing intensity to be plotted as a function of 1/𝑑, where 𝑑 is the Bragg interplanar spacing.

3. Results

Our analysis assumes random grain nucleation within the amorphous matrix [16]. Lateral grain growth commences upon nucleation, proceeding until impingement of the grain onto other grains. In several repeated trials, we observed the onset of rapid grain nucleation within several seconds of reaching 250C. Nearly complete crystallization occurred within 2.5 minutes after the onset of nucleation (Figure 1).

In classical solid-state phase change theory, the variation of 𝑋𝑐 with 𝑡 during 2D grain growth is described by

𝑋𝑐(𝑡)=1exp𝑡𝑡0𝑡𝑐3,(1) for 𝑡𝑡0, where 𝑡0 is the incubation time and 𝑡𝑐 is a characteristic crystallization time.

Assuming a nucleation rate 𝑟𝑛, the variation of 𝜌𝑔 with 𝑡 for 𝑡𝑡0 follows

𝜌𝑔(𝑡)=𝜋𝑟𝑛𝑡𝑐6𝐸3𝑡𝑡0𝑡𝑐,(2) using the generalized error function:


Leastsquares fitting of the measurements of 𝑋𝑐(𝑡) and 𝜌𝑔(𝑡) were combined into a single, multivariate data set, which was fit simultaneously to (1) and (2), by varying the parameters 𝑡0, 𝑡𝑐, and 𝑟𝑛 (Figure 2).

The high quality of fit supports the validity of the applied model. The grain-growth velocity 𝑠𝑔 is computed from

𝑠𝑔=3𝜋𝑟𝑛𝑡𝑐31/2.(4) The average grain size is estimated from the assumption of cylindrical grain shapes, having the cylinder axis normal to the film plane, which project to circular profiles in plan-view examination. Extrapolation to 𝑡 gives the final, average grain size:

𝑑𝑔𝑠()=1.20𝑔𝑟𝑛1/3,(5) using 2(3/𝜋)1/3Γ(1/3)1.20. The columnar grain morphology assumed is applicable to larger grains (greater than 100 nm), for which little overlap is evident in plan-view projection. However, the presence of smaller grains, which often overlap the larger grains in projection, may lead to a slight underestimate of the average, final grain size.

Calculated values of 𝑟𝑛, 𝑠𝑔, and 𝑑𝑔() are tabulated in Table 1. Based on the measurements of kinetic parameters at intermediate stages of crystallization, a value of 𝑑𝑔()=0.30𝜇m is predicted. This value is consistent with actual grain sizes seen in Figure 1, which range from tens of nm to nearly 1 𝜇m.


𝑡 𝑐 1 2 0 ± 4 s
𝑟 𝑛 ( 1 . 3 1 ± 0 . 1 1 ) × 1 0 9 1/( s n m 3 )
𝑠 𝑔 2 . 0 3 ± 0 . 0 9 nm/s
𝑑 𝑔 ( ) 3 0 0 ± 1 0 nm

The data set analyzed here was selected, based on the high image quality, from among several comparable data sets. However, the crystallization in all of the samples annealed under identical conditions transpired in a quantitatively similar fashion to that presented, resulting in comparable grain morphology and size. Note that each annealing treatment resulted in the simultaneous crystallization of the entire sample, though the area imaged by TEM was typically less than 25 𝜇m2, leaving a vast majority of each sample unobserved during transformation.

Diffraction patterns (Figure 3) clearly show the transition from the as-deposited, amorphous state to the final, crystallized state. The diffraction-ring positions of fully crystallized films are consistent with the anatase phase (space group 𝐼41/𝑎𝑚𝑑, no. 141), [17], based on a comparison with kinematic electron-diffraction simulations using EMS online software [18]. We note differences in relative intensities, particularly the presence of the kinematically forbidden 200 diffraction ring, which can arise from dynamical scattering, and may also be influenced by double diffraction, planar-defect structure, and preferential orientation. Analysis using convergent-beam electron diffraction may elucidate the origins of these features.

4. Conclusion

The crystallization kinetics of as-deposited a-TiO2 films on amorphous substrates were analyzed in terms of classical phase-transformation theory, assuming spontaneous, homogeneous grain nucleation throughout the film volume and isotropic grain growth. Several subsequent experiments are planned: ( 1) measurement of thermal activation of grain nucleation and grain growth, by studying variations with annealing temperature; ( 2) characterization of the crystallized grain structure, including defect character, preferential orientation, and dependence of growth velocity on crystallographic direction; ( 3) electron-diffraction analysis during crystallization using TEM in situ annealing.


This work was supported by the U.S. Department of Energy, project no. DOE DE-FG02-08ER64624, and by the National Science Foundation, project no. 0453216.


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Copyright © 2009 J. C. Johnson et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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