Morphology and Photoluminescence of HfO2Obtained by Microwave-Hydrothermal
© to the authors 2009
Received: 26 June 2009
Accepted: 22 July 2009
Published: 13 August 2009
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© to the authors 2009
Received: 26 June 2009
Accepted: 22 July 2009
Published: 13 August 2009
In this letter, we report on the obtention of hafnium oxide (HfO2) nanostructures by the microwave-hydrothermal method. These nanostructures were analyzed by X-ray diffraction (XRD), field-emission gum scanning electron microscopy (FEG-SEM), transmission electron microscopy (TEM), energy dispersive X-ray spectrometry (EDXS), ultraviolet–visible (UV–vis) spectroscopy, and photoluminescence (PL) measurements. XRD patterns confirmed that this material crystallizes in a monoclinic structure. FEG-SEM and TEM micrographs indicated that the rice-like morphologies were formed due to an increase in the effective collisions between the nanoparticles during the MH processing. The EDXS spectrum was used to verify the chemical compositional of this oxide. UV–vis spectrum revealed that this material have an indirect optical band gap. When excited with 488 nm wavelength at room temperature, the HfO2nanostructures exhibited only one broad PL band with a maximum at around 548 nm (green emission).
Currently, the researches in nanoscience have been especially dedicated to the development of synthesis routes with ability for the formation of new nanostructured materials with distinct structural and morphological characteristics . In principle, the chemical and physical properties of nanostructured oxide with well-defined morphologies are technologically more interesting because they differ from those in the bulk shape. For example, the porous CuO hollow structures as well as the Nb2O5 nanotubes are particularly attractive due to its applications in catalysis, Li+ ion batteries and sensors [2–4].
In the last years, the hafnium oxide (HfO2) has been extensively investigated as an alternative material to replace the silicon dioxide employed in gate dielectric systems of microelectronic devices [5–9]. Moreover, this material has a wide potential for the fabrication of complementary metal–oxide–silicon transistors with small dimensions and/or liquid crystals because of its high-K dielectric constant, relatively low leakage current, wide band gap (5.70 eV), good thermal stability, and high transparency [10–15]. Recently, different nano-sized particle materials (gold, cobalt, platinum, and germanium) have been embedded into the HfO2 matrix to improve the interfacial and electrical properties of metal–oxide–semiconductor capacitors [16–19].
The optical properties of pure or doped HfO2 have been mainly focused on the photoluminescence, cathode-luminescence, and scintillation measurements [20–22]. For example, Rastorguev et al.  performed both photoluminescence and cathode-luminescence measurements on as-deposited HfO2 films and on those heat treated at 800 °C for 30 min. The two broad PL bands detected in these films were attributed to the self-trapped excitons due to the presence of oxygen vacancies. Chang et al.  reported on the PL behavior of germanium nanocrystals embedded in HfO2 and HfAlO structures. The differences observed between the PL spectra of these two samples were explained by the quantum confinement barrier. Taniguchi et al.  observed in Eu3+-doped HfO2 nanoparticles a broad photoluminescence (PL) band covering from ultraviolet to visible region of the electromagnetic spectrum as well as the characteristic transitions of Eu3+ ions. According to these authors, the broad PL band originates from electron-hole recombination via surface defect centers. Also, Ni et al.  described that the PL emissions of HfO2 films are controlled by the concentration of oxygen vacancies into the lattice.
In terms of structural characteristics, the HfO2 presents a monoclinic structure with space group P 21/c in the range from room temperature up to 1,700 °C [25, 26]. The increase of temperature up to 2,600 °C promotes a phase transition from monoclinic (P 21/c) to tetragonal structure (P 42/nmc), reducing the unit cell volume to approximately 3.5% [27, 28]. Above 2,600 °C, this compound exhibits a fluorite-type cubic structure with space group . According to the literature [29, 30], this high temperature cubic phase can be stabilized at room temperature doping the HfO2 lattice with Y3+ ions.
The literature has reported the preparation of pure or doped HfO2 (nanoparticles, powders, or films) by different synthetic routes, mainly including: alkoxide in solvents non-aqueous , non-hydrolytic sol–gel , solvent casting with oxo-clusters , non-aqueous sol–gel with atomic layer deposition , conventional hydrothermal (CH) [35–37], ultrasonically assisted hydrothermal , pulsed laser deposition , plasma-assisted chemical vapor deposition , and solvothermal [41, 42]. In particular, the CH is an interesting synthesis method due to the formation of different oxides with a good control on the morphology and particle sizes, high degree of crystallinity, and easy dispersion in aqueous medium . Although this method can be efficient in the preparation of materials using low heat treatment temperatures, its main drawback is related to the long processing times. In order to overcome this problem, Komarneni and Katsuki  innovated the CH systems through the use of microwave radiation. The development of this new system, known as microwave-hydrothermal (MH) [45, 46], promoted an increase in the kinetics of crystallization by 1 or 2 orders of magnitude, drastically reducing the processing times for minutes or some hours during the synthesis. These advantages are arising from the direct interaction between the microwave-radiation with the atoms, ions, and/or molecules of the aqueous medium and/or dispersed phase . In this case, this interaction induces a molecular rotation because of the permanent or induced dipole alignment with the oscillating microwave electric field (frequency of 2.45 GHz) . This phenomenon promotes a transformation from rotational energy to heat, which is necessary for the formation and crystallization of the particles. Therefore, in this letter, we report on the obtention of rice-like HfO2 nanostructures by the MH method.
The structural and morphological properties were characterized by means of X-ray diffraction (XRD), field-emission gun scanning electron microscopy (FEG-SEM), transmission electron microscopy (TEM), and energy dispersive X-ray spectrometry (EDXS). The optical properties were analyzed through ultraviolet–visible (UV–vis) absorption spectroscopy and photoluminescence (PL) measurements.
The rice-like HfO2nanostructures were structurally characterized by X-ray powder diffraction (XRD) using a Rigaku-DMax/2500PC (Japan) with Cu–Kα radiation (λ = 1.5406 Å) in the 2θ range from 20° to 80° with scanning rate of 0.02°/min. The morphologies were investigated through a FEG-SEM (Supra 35-VP, Carl Zeiss, Germany) operated at 6 keV and with a TECNAI G2 TEM (FEI Corporation, Holland) operated at 200 keV. UV–vis spectra were taken using a Cary 5G (Varian, USA) spectrophotometer in diffuse reflection mode. PL measurements were performed using a U1000 (Jobin-Yvon, France) double monochromator coupled to a cooled GaAs photomultiplier with a conventional photon counting system. An argon ion laser (λ = 488 nm) was used as excitation source, keeping its maximum output power at 25 mW. UV–vis and PL spectra were taken three times for each sample to ensure the reliability of the measurements. All measurements were performed at room temperature.
Atomic coordinates used to model the HfO2unit cell
As it can be seen in this table, the lattice parameters obtained in this work are very close to the reported in the literature [54–56]. However, the small differences observed between these values can be related to the synthesis methods. Therefore, we believe that the experimental conditions (heat treatment temperature, heating rate, and/or processing time) employed in the synthesis methods to obtain the HfO2 (film or powder) are able to promote the formation of particles with several morphologies and different sizes, probably inducing residual stresses, and/or distortions into the lattice .
Comparative results between the optical band gap energy of rice-like HfO2nanostructures obtained in this work with those reported in the literature by other methods
FEG-SEM micrograph indicated the presence of several rice-like HfO2 nanostructures with agglomerate and polydisperse nature (Fig. 3a). The high magnification FEG-SEM micrographs showed that these morphologies are composed of several primary particles (Fig. 3b, c). In fact, probably the Brownian motion of these particles in suspension resulted in collision events between them . Hence, we believe that the microwave radiation intensified the effective collision rates of the primary particles. In principle, when two nanoparticles collide with the same crystallographic orientation, the adhesion process occurs with highest probability. This probability is slightly reduced when the nanoparticles are not aligned. After this phenomenon, the nanoparticles remain in contact by Van der Waals forces and the coalescence process takes place, resulting in the formation of rice-like morphologies. This conclusion can be confirmed by means of low magnification TEM micrographs in Fig. 3d and e, where it was verified that these morphologies are formed by several aggregated nanoparticles. Also, in these micrographs, the bright areas correspond to the individual nanoparticles, while the black areas indicate the regions with stacking between the nanoparticles oriented in different crystallographic planes. The EDXS analysis revealed that the nanoparticles are chemically composed of Hf and O atoms. Therefore, this result suggests that the MH conditions performed at 140 °C for 1 h lead to the formation of pure HfO2 phase (Inset in Fig. 3e). The presence of Cu atoms in the spectrum is arising from the carbon-coated copper grids. Figure 3f shows a high magnification TEM micrograph of an individual HfO2 nanoparticle chosen in Fig. 3e (black rectangle). On this selected region, it was performed a HR-TEM micrograph as well as a Fourier-transform. In the Fourier-transform, the respective crystallographic planes were estimated by the FTL-SE program (version 1.10 for Windows) (http://www.jcrystal.com/jcrystal.html). The interplanar spacing was determined in approximately 3.12 Å by means of the HR-TEM micrograph, which correspond to the ( ) crystallographic plane. The Fourier-transform confirmed that these morphologies present a single phase with monoclinic structure. According to Debye scattering equation described in the literature [42, 61], the preferential growth direction of these morphologies occurs along the  direction.
Recently, Mohanty and Landskron  observed this same morphology in periodic mesoporous organosilica synthesized by the template assisted sol–gel method using a chain-type precursor. According to these authors, this morphology is a kind of mesostructure formed by periodic one-dimensional channels, containing pore sizes of ca. 4 nm and channel wall diameters of ca. 6 nm.
where y0 is the first value in y-axis, A is the amplitude, w is the width, π is a constant, xc is the center value of the distribution curve in x-axis. Thus, the distribution is asymmetrical on the logarithmic scale of average particle size [63, 64]. Figure 4a shows the average particle width distribution in the range from 15 to 75 nm for the rice-like HfO2 nanostructures. In this case, it was noted that approximately 81% particles presented an average width between 35 and 55 nm. On the other hand, approximately 77% particles exhibited an average height in the range from 85 to 105 nm. Possibly, the differences observed between width and height is caused by the increase in the effective collision rates between the nanoparticles by the microwave radiation, as previously described in the text.
where α is the absorbance, h is the Planck constant, ν is the frequency, Egap is the optical band gap, and n is a constant associated to the different electronic transitions ( 2, or 3 for direct allowed, indirect allowed, direct forbidden, and indirect forbidden transitions, respectively). According to Park et al.  and Ramo et al.  the monoclinic HfO2 structure presents an indirect band gap. In principle, the band gap energy is considered indirect when the electronic transition occurs from maximum-energy states near or in the valence band to minimum-energy states below or in the conduction band, but in different regions in the Brillouin zone  (Inset in Fig. 5b). Based on these information, the Egap of HfO2 nanoparticles was calculated using n = 2 in Eq. 5 and extrapolating the linear portion of the curve or tail. The obtained result indicated an Egap value at around 3.31 eV (Fig. 5a), which is lower than those reported in the literature by means of experimental methods or theoretical calculations [69–72]. A plausible explication for this phenomenon can be the existence of several intermediary energy levels within the band gap, as consequence of the symmetry break (oxygen vacancies) and/or distortions on the [HfO6 clusters because the influence of microwave radiation. It is possible that these energy levels are basically composed of oxygen 2p states (near the valence band) and hafnium 5d states (below the conduction band) .
Results obtained by the deconvolution of the PL spectrum of rice-like HfO2nanoparticles formed by MH at 140 °C for 1 h
In this table, it was observed that the smallest area is associated to the cyan light emission component (P1peak). Therefore, this result suggests that there is a lower contribution of the shallow holes for the PL spectrum. On the other hand, the green and orange light components (P1, P2, P3, and P4) are related to the deep holes, which are predominant in the PL behavior.
In the last years, investigations performed through the electron paramagnetic resonance (EPR) technique in HfO2 bulk have shown the existence of Hf3+ defects into the structure, acting as charge trapping centers. These defects were detected near or on the HfO2 surface, suggesting that they are a kind of oxygen vacancy . Although the oxygen vacancies can be considered key factors in the PL behavior of HfO2, possibly in our case, the distortions on the [HfO6 clusters caused by the interaction with the microwave radiation contributed for the formation of intermediary energy levels (deep and shallow holes) within the band gap. On the basis of this hypothesis, inset in Fig. 5b shows 12 different bond angles values for the [HfO6 clusters. The bond angles were qualitatively estimated by the Java Structure Viewer program (http://www.jcrystal.com/steenweber/JAVA/JSV/jsv.html), considering the crystallographic data displayed in Table 2. In principle, future investigations based on both experimental data and theoretical calculations will be necessary to a better understanding on the intermediary energy level distribution and nature of the structural defects as well as provide information on its origins within the band gap of HfO2.
In summary, rice-like HfO2nanostructures were obtained by the MH method at 140 °C for 1 h. XRD patterns revealed that this oxide crystallizes in a monoclinic structure with space groupP 21/c without the presence of secondary phases. FEG-SEM and TEM micrographs indicated that the MH processing favored the formation of rice-like HfO2nanostructures with agglomerate and polydisperse nature. These morphological characteristics were attributed to the effective collision rates between the primary particles by the microwave radiation and due to its mutual interactions by Van der Waals forces. These nanostructures exhibited an average width in the range from 15 to 75 nm as well as an average height between 85 and 105 nm. The UV–vis absorption spectrum showed anEgapvalue of 3.31 eV, which was ascribed to the presence of intermediary energy levels between the valence band and conduction bands (deep and shallow holes) within the band gap. The PL behavior was related to the existence of oxygen vacancies and/or distortions on the [HfO6] clusters into the lattice.
The authors thank the financial support of the Brazilian research financing institutions: CAPES, CNPq, and FAPESP. Special thanks to W. J. Botta Filho and A. M. Jorge Jr. by the TEM measurements, Dr. C. S. Xavier by their valuable discussions and also to Dr. D. P. Volanti by the development of the microwave-hydrothermal system.