Elsevier

Vibrational Spectroscopy

Volume 54, Issue 2, 18 November 2010, Pages 89-92
Vibrational Spectroscopy

Raman spectroscopy as a tool for the elucidation of nanoparticles with core–shell structure of TiO2 and MoO3

https://doi.org/10.1016/j.vibspec.2010.03.010Get rights and content

Abstract

In this work, we report the synthesis of TiO2 nanoparticles and core–shell TiO2–MoO3 and MoO3–TiO2 nanoparticles dispersed into porous Vycor glass by the metallo-organic decomposition process (MOD). The nanoparticles were analyzed using Raman spectroscopy by monitoring the E2g band (phonons region for anatase TiO2) and the bands located at 820 and 996 cm−1 (vibrational modes of α-MoO3) when Mo is present. The diameters of the TiO2 nanoparticles dispersed in the glass matrix were calculated by means of the phonon confinement model and the values obtained are 3.9, 4.6, and 5.7 nm depending on the number of impregnation–decomposition cycles used in the nanoparticle syntheses.

Introduction

In recent years, much of the research in nanomaterials has focused on semiconductor nanoparticles, since the nanoparticles display a variety of fundamentally interesting physical and chemical properties resulting directly from their size and dimensionality. Semiconductor based core–shell nanoparticles (CSN) represent an important type of advanced material, since their properties can be tailored to suit applications such as modulation of optical properties [1], [2], magnetism [3], [4], heterogeneous catalysts [5], [6], and solar energy conversion [7], [8].

Nanocrystalline anatase TiO2 is a potential material for photocatalytic applications [9]. However, its large band gap of 3.2 eV (outside the most intense region of the solar spectrum, centered at 2.6 eV) is a problem that researchers must overcome. To make TiO2 suitable for practical solar energy conversion, materials on the nanometer scale with core–shell structure have been synthesized [10], [11]. Another approach is the combination of anatase TiO2 and orthorhombic α-MoO3 (band gap of 2.9 eV), that could result in heterostructured materials with band gaps of ca. 2.7 eV, due to the arrangements of the valence and conduction bands.

Among the various techniques that can be used for the characterization of nanostructures, Raman spectroscopy is presented as a potential tool, since it provides important information about connectivities in those materials [12], [13], [14], [15]. Theoretically, the fundamental q  0 Raman selection rule is relaxed for a finite-size domain, allowing participation of phonons away from the Brillouin zone center [16]. The phenomenon of spatial confinement of optical phonons was studied by Richter et al. [17]. It was shown that the Raman spectra of nanocrystalline semiconductors are red-shifted and broadened due to the relaxation of the q-vector selection rule in finite-size nanocrystals. The phonon uncertainty is Δq  1/d, where d is the diameter of a nanocrystal or quantum dot. This spatial confinement inside nanocrystals gives rise to a shift and to an asymmetric broadening of the Raman band in nanostructures compared to bulk crystals [18], [19]. The phonon confinement effects in the Raman scattering of TiO2 nanocrystals have been studied [20], [21], but due to the large number of polymorphs of molybdenum oxide, its study by the phonon confinement model becomes difficult.

In this work, we report the synthesis of core–shell nanoparticles of titanium and molybdenum oxides produced by metallo-organic decomposition process in a porous matrix. The samples were analyzed by Raman spectroscopy.

Section snippets

Synthesis of core–shell nanoparticles of TiO2 and MoO3

The TiO2–MoO3 and MoO3–TiO2 core–shell nanoparticles dispersed in porous Vycor glass (PVG, Corning Glass®) were prepared by the metallo-organic decomposition process, which consists in impregnation followed by decomposition of the titanium (IV) and molybdenum (VI) precursors. PVG was impregnated with titanium (IV) di-(propoxy)-di-(2-ethylhexanoate), Ti(Prop)2(Hex)2, or molybdenum (VI) 2-ethylhexanoate, Mo(Hex)6. These metallo-organic compounds were thermally decomposed under air at 1023 K for 8 h

Results and discussion

PVG/xTiO2 with x = 3, 5 and 7 were analyzed using Raman spectroscopy under the same analysis conditions. The bulk anatase TiO2 spectrum is presented for comparison (Fig. 1) and shows two intense bands located at ca. 144 and 638 cm−1 [21], [22]. The spectrum of pure PVG, characterized by broad bands typical of vitreous materials [21], is also presented. The presence of anatase TiO2 related Raman bands in PVG/xTiO2 samples is indicative of the titania phase present inside PVG. The most intense band

Conclusions

In this work, we report the synthesis of a series of TiO2–MoO3 and MoO3–TiO2 nanoparticles inside porous Vycor glass. Raman spectroscopy shows that this synthesis method allows to control the preparation of core–shell nanoparticles in the Vycor® glass pores. The size-dependent Raman spectra band shifts are explained based on the phonon confinement model. A detailed analysis of the behavior of the E2g band of the anatase TiO2 and of the bands attributed to α-MoO3 supplies important information

Acknowledgements

The authors are grateful to FAPESP and CNPq for financial support, to Prof. D.L.A. Faria and Prof. M.L.A. Temperini (IQ-USP, São Paulo, Brazil) and Prof. A.G. Souza Filho (UFC, Brazil) for assistance with the Raman measurements, and to Prof. C.H. Collins (IQ-UNICAMP, Brazil) for English revision. This is a contribution of National Institute of Science and Technology in Complex Functional Materials—Inomat (CNPq-MCT/FAPESP).

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