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Advances in Materials Science and Engineering
Volume 2009 (2009), Article ID 502437, 4 pages
http://dx.doi.org/10.1155/2009/502437
Research Article

Structural and Raman Vibrational Studies of - Oxide System

1Laboratoire Matériaux et Environnement LME, Faculté des Sciences, Université Ibn Zohr, BP 8106, Cité Dakhla, 80000 Agadir, Morocco
2Institut Matériaux Microélectronique et Nanosciences de Provence, IM2NP, UMR CNRS 6242, Université du Sud Toulon-Var, BP 20132, 83957 La Garde Cedex, France

Received 10 August 2009; Accepted 1 November 2009

Academic Editor: Peter Majewski

Copyright © 2009 L. Bourja 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.

Abstract

A series of ceramics samples belonging to the - phase system have been prepared via a coprecipitation route. The crystallized phases were obtained by heating the solid precursors at for 6 hours, then quenching the samples. X-ray diffraction analyses show that for a solid solution with fluorine structure is formed. For x ranging between 0.25 and 0.7, a tetragonal phase coexisting with the FCC solid solution is observed. For x ranging between 0.8 and 0.9, a new tetragonal phase appears. The phase is postulated to be a superstructure of the phase. Finally, close to , the classical monoclinic structure is observed. Raman spectroscopy confirms the existence of the phase changes as x varies between 0 and 1.

1. Introduction

In the past, several systems based on cerium dioxide CeO2 (ceria) were extensively investigated for their electrochemical, conduction, or catalytic properties [115]. Nanostructured powders of pure and doped ceria can be obtained in various ways [16, 17]. In the present work we deal with the bismuth cerium oxide system CeO2-Bi2O3. This system might be of a high interest for catalytic applications and integration in gas sensors. At present, the cerium bismuth oxide phase diagram (CeO2-Bi2O3) is not well known. For low Bi fractions, it was clearly established that a solid solution was formed. The substituted phase with (where oxygen vacancies are noted V) is cubic and its cell parameter increases with x because of size of Bi3+ ionic radius:  nm and  nm [18, 19]. However, above the composition , the nature of phases is not well known. In the present work, we describe a new series of observed phases prepared via a coprecipitation route and after heating at C.

2. Experimental

Fourteenth polycrystalline samples were prepared by mixing bismuth and cerium nitrates solutions (Bi(NO3)3, 5H2O + Ce(NO3)3, 6H2O) and adding NH4OH [20, 21] to obtain precipitation of NH4NO3 and bismuth cerium hydroxides. Bismuth compositions ranged from 0% Bi to 100% Bi. The solid obtained by coprecipitation was then heated under air at C for 6 hours. Experiments carried out at intermediate heating times showed that the observed crystallized phases appear as being stable above heating times of 2 hours.

3. Results

The polycrystalline samples were analyzed by X-ray diffraction, using a D5000 Siemens-Bruker diffractometer, equipped with a copper X-ray source (wavelength  m; tension  kV, intensity  mA), and with a monochromator eliminating radiation. The analyses were carried out using the classical -2 configuration, with 2 angle steps of and counting times of 19 s per step. Raman spectroscopy was used to characterize the observed various phases. A micro-Raman system Horiba. Jobin-Yvon Labram HR 800 equipped with argon laser source (Raman wavelength  nm) was used to observe the various vibrational spectra. All spectra were acquired with a recording time of 30 seconds.

3.1. Structural Studies

X-ray diffraction shows that a strong evolution occurs in the phase system as bismuth atom fraction increases. Figures 1(a), 1(b), 1(c), and 1(d) show the X-ray diffraction patterns for samples noted ( )CeO2, /2Bi2O3 with x varying between 0 and 1. The cell parameters of substituted samples noted as were refined. From to , the cell parameters linearly vary with :  nm; ; ; ; .

fig1
Figure 1: XRD patterns ( ) of pure samples CeO2, Bi2O3 heated at C. (a) XRD patterns for ; (b): XRD patterns for biphasic system; (c) and 0.9; (d)    - Bi2O3.

Above the composition , a multiphase system is evidenced and the ceria-based phase presents a constant cell parameter nm: the two new additional phases are identified as being tetragonal and closely related to bismuth oxide structural varieties: their cell parameters were refined. In the composition range from 0.3 to 0.7, a tetragonal phase is observed with refined cell parameters: ; . It is a superstructure of the tetragonal phase observed for compositions , with refined cell parameters: ; . These substituted phases were never observed, and testing structural models are in progress to better describe these phases.

3.2. Vibrational Studies

raman spectroscopy data are reported on Figures 2(a) and 2(b): in Figure 2(a), the solid solution ( ) is characterized by a main vibrational band at 460–465  with complementary small bands at 520–590  associated with the presence of Bi3+ and oxygen vacancies in the cubic lattice. In Figure 2(b) the Raman spectra of other samples are represented for compositions ranging between 0.3 and 1. The vibration bands are increasingly more complex as Bi composition increases. The cubic phase of CeO2 is well characterized by the 465  Raman band. In the composition range from to 0.20 the bands located at 462–516–595  might be associated with the solid solution . The additional bands are underlined and should be linked to presence of Bi3+ ions and vacancies (clusters Bi3+-V-Bi3+). In the range to 0.70, the Raman bands 460, 520, 590, 94, 126, 316, 530 (in cm-1) might be related to the biphasic system: cubic solid solution + tetragonal superstructure ’. In the range to 0.90, a new biphasic system associated with the bands 95, 120, 315, 450, 538 (tetragonal phase) and 70, 85, 140, 152, 184, 212, 285, 418, 630 (monoclinic lattice) is observed: these vibration bands could characterize the system “Tetragonal Monoclinic ” Finally for the Bi2O3 sample, the standard monoclinic structure is observed.

fig2
Figure 2: Raman spectra ) of bismuth cerium oxide phases, CeO2, /2. Bi2O3; (a) solid solution for to 0.25; (b) multiphase system for to 1. Raman shift island are in , values from 0 to 1. The bands at 520 and 590  are linked to structural defects.

4. Conclusions

New correlations between XRD data and Raman spectroscopy have been established for the system CeO2-Bi2O3. From samples prepared at C, a partial phase diagram is proposed with the probable existence of at least 4 domains. The X-ray diffraction and Raman spectroscopy analyses clearly show that phase changes occur at C, with at least (i) a solid solution domain (cubic phase), (ii) a biphasic domain (tetragonal phase rich in bismuth coexisting with the cubic phase), (iii) a biphasic system with coexistence of two and tetragonal phases, the phase being highly rich in bismuth), and finally (iv) a biphasic domain in which monoclinic and tetragonal phases coexist. The solid solution can be represented from the basic CeO2 face-centered cubic lattice. The tetragonal phase can be represented by a cell built on the ceria fcc structure, with lattice vectors ( ): this structure was previously observed in the literature as a tetragonal variety of pure or non stoichiometric Bi2O3 phase [22, 23]. The Bi rich phase ( ) having the superstructure noted can be represented by a cell built on lattice vectors ( ). The observed pure Bi2O3 phase is monoclinic. The effective compositions of the and new cerium bismuth phases are not clearly known and new studies using transmission electron microscopy analyses are in progress.

Acknowledgment

The authors gratefully acknowledge the Provence-Alpes-Côte d’Azur Regional Council, the General Council of Var, and the agglomeration community of Toulon Provence Mediterranean for their helpful financial support in 2007 and 2008.

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