Influence of Fe3+-doping on optical properties of CeO2−y nanopowders
Introduction
Ceramic materials based on cerium oxide (ceria, CeO2) have been a very active research field in the area of photocatalytic technologies such as production of oxygen trough water decomposition [1] and photodegradation of toluene in gas phase [2], methylene blue [3], acidic black 10b [4] and acid orange 7 [5] industrial dyes. The recent study of Ji et al. [5] have revealed that nanophased CeO2 is more efficient photocatalyst in the visible region for dye wastewater treatment than the commercial TiO2 [5]. Doping with transition metals, such as Fe, enhances the oxygen mobility and oxygen storage capacity of ceria lattice [6] which can improve photocatalytic properties of CeO2 nanomaterials [3]. Also Fe-doped ceria nanoparticles were used for pigmented ultraviolet filter applications [7]. The optimization of photocatalytic technologies which utilize solar radiation is directed towards the development of ceria materials with precisely controlled position of the absorption edge and tunable electronic band structure.
Even though extensive research has been performed on the optical properties of ceria based nanomaterials, still a lot of controversy exists in the literature regarding the nature of the optical band gap transition (Eg) which corresponds to the O 2p→Ce 4f transition. Guo et al. [8] reported the optical band gap values of 3.6 eV and 3.3 eV for direct and indirect transitions respectively, in a case of bulk (crystalline film) ceria sample. A certain number of authors [9], [10], [11], [12] have calculated the optical band gap of various ceria based materials, treating it as a direct transition. Contrary to them, a group of other authors [13], [14], [15], [16], [17] ascribed the optical band gap of CeO2 to the indirect transition. Independent measurements performed on oxygen deficient ceria structures using non optical techniques, gave the values of 3.3 eV [18], and 3.4–3.6 eV [19] without defining the type of the transition. The present uncertainty in the band gap calculations of nanostructured CeO2−y increases a need for better explanation of its electronic properties using sophisticated analytical models which incorporate nanosized ceria defective structure.
The decrease of the particle size to nanodimensions leads to the increase of the band gap energy in majority of materials due to the quantum confinement effects [20]. In a case of nanoceria an anomalous behavior in the band gap energy was observed for the grain size less than 20 nm [9]. The decrease of the band gap energy with grain size decrease can be explained by a transformation from the crystalline into the amorphous state when crystals become of nanodimension [9] and increase in the number of defects within the band gap [16]. All these nano-size related effects are reflected in the spectral dependence of the complex dielectric function which is, through its imaginary part (ε2(E)), related to the energy-band structure. Being a nondestructive and very sensitive technique, spectroscopic ellipsometry (SE) represents a very convenient method for precise and direct determination of the complex dielectric function of nanostructured materials from which important information about materials electronic structure can be obtained.
The aim of this work was to investigate the influence of Fe3+-doping on the optical properties and band gap behavior of CeO2−y nanopowders. We applied different ellipsometric models in order to deduce which model describes best the electronic properties of nonstoichiometric pure and Fe3+-doped CeO2−y.
Section snippets
Experiment
Non-stoichiometric nanopowders of pure CeO2−y (coefficient y denotes the oxygen deficiency and for small particles ranges from 0–0.2 [21], [22]) and CeO2−y doped with 1 mol%, 3 mol% and 5 mol% of trivalent iron ions were synthesized by the hydrothermal method using NH4OH solution and relatively low calcination temperature (200 °C). Detailed preparation procedure is published elsewhere [23].
The X-ray diffraction (XRD) patterns were collected using Rigaku RINT2200 powder diffractometer. Non-contact
Analytical models
From the measurements of ellipsometric angles Ψ and Δ, by using the two-phase model approximation (CeO2−y nanoparticles/air), we have calculated the pseudo-dielectric function spectra directly from the complex reflectance ratio ρ(E)=tan Ψexp(iΔ) using the relation [24]where θi is the incidence angle. Measurement of pseudo-dielectric function enables direct determination of real and imaginary part of the complex dielectric function spectrum ε(E)=ε1(Ε)+iε2(Ε).
Results and discussion
In Fig. 1 are given the XRD spectra of pure and Fe3+-doped CeO2−y samples. All synthesized samples have fluorite type crystal structure of cerium dioxide and no secondary phase was detected. Characteristic Miller indices are denoted for each diffraction peak.
Significant broadening of the peaks indicates that investigated powders consist of nanometric size crystallites. The crystallite size D of the samples was estimated from XRD data by taking into account strain contribution, using the
Conclusion
The hydrothermal method has been employed to synthesize ceria nanopowders doped with iron. XRD analysis showed that all investigated samples have fluorite cubic crystal structure with particle size in nanometric range, confirmed by NC-AFM results. From Raman spectroscopy measurements we have observed an increase of oxygen vacancies concentration with increasing amount of Fe up to 3 mol%. In the Raman spectrum of Ce0.95Fe0.05O2−y sample, the formation of iron oxide wüstite (FeO) phase was
Acknowledgment
This work was financially supported by the Serbian Ministry of Education and Science under the Projects ON171032 and III45018, Swiss National Science Foundation through Grant IZ73Z0-128169 and Serbian-Spanish bilateral project through Grant AIB2010SE-00160.
References (45)
- et al.
Structural characterization and photocatalytic behaviors of doped CeO2 nanoparticles
Journal of Alloys and Compounds
(2009) - et al.
Preparation, characterization and photocatalytic activity of CeO2 nanocrystalline using ammonium bicarbonate as precipitant
Materials Letters
(2007) - et al.
Study of adsorption and degradation of acid orange 7 on the surface of CeO2 under visible light irradiation
Applied Catalysis B
(2009) - et al.
Fe-doped ceria solids synthesized by the microemulsion method for CO oxidation reactions
Applied Catalysis B
(2011) Structure, microstructure and optical properties of cerium oxide thin films prepared by electron beam evaporation assisted with ion beams
Solid State Sciences
(2009)- et al.
Optical constants of nanocrystalline lanthanide-doped ceria thin films with the fluorite structure
Journal of Physics and Chemistry of Solids
(1998) - et al.
Journal of Materials Science and Engineering
(2003) - et al.
Effects of ion irradiation and annealing on optical and structural properties of CeO2 films on sapphire
Physica B
(2007) - et al.
The electronic structure of stoichiometric and reduced CeO2 surfaces: an XPS, UPS and HREELS study
Surface Science
(1994) - et al.
Cerium oxidation state in ceria nanoparticles and absorption near edge spectroscopy
Surface Science
(2004)
Optical characterization of amorphous slicon hydride films
Solar Cells
X-ray line broadening from filed aluminium and wolfram
Acta Metallurgica
The size and strain effects on the Raman spectra of Ce1−xNdxO2−δ (0<x<0.25) nanopowders
Solid State Communications
Structural and magnetic study of Fe-doped CeO2
Physica B
Effect of iron doping and annealing on structural and optical properties of cerium oxide nanocrystals
Journal of Physics and Chemistry of Solids
The photocatalytic oxidation of water to O2 over pure CeO2, WO3, and TiO2 using Fe3+ and Ce4+ as electron acceptors
Applied Catalysis B
Synthesis, characterization and computational study of nitrogen-doped CeO2 nanoparticles with visible-light activity
Physical Chemistry Chemical Physics
Synthesis and characterization of Fe doped CeO2 nanoparticles for pigmented ultraviolet filter applications
Journal for Nanoscience and Nanotechnology
A spectroscopic–ellipsometry study of cerium dioxide thin films grown on sapphire by rf magnetron sputtering
Journal of Applied Physics
Microstructure-property relationships in nanocrystalline oxide thin films
Ionics
Preparation of monodispersed nanocrystalline CeO2 powders by microwave irradiation
Chemical Communications
Morphology-controllable synthesis of mesoporous CeO2 nano- and microstructures
Chemistry of Materials
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