Electronic and structural properties of La0.4Sr0.6Ti1−yCoyOδ electrode materials for symmetric SOFC studied by hard X-ray absorption spectroscopy

https://doi.org/10.1016/j.ijhydene.2013.05.005Get rights and content

Highlights

  • XANES/EXAFS reveal invariance of the local structure and formal valence of Ti in LSTC.

  • Dramatic changes at the Co-site are produced with increasing Co content.

  • Stability of Ti4+ triggers the formation of A-site vacancies in LSTC materials.

  • The reduction of A-site deficiency with increasing Co content in LSTC is explained.

  • An improved electrochemical performance for higher Co content is predicted.

Abstract

We present combined Synchrotron X-ray Absorption Near Edge Spectroscopy (XANES) and Extended X-ray Absorption Fine Structure (EXAFS) study of La0.4Sr0.6Ti1−yCoyOδ (0 ≤ y ≤ 0.5), which are promising electrode materials for symmetric solid oxide fuel cells. The measurements were performed at room temperature at the Ti and the Co K-edges in order to determine the local structural and electronic changes around the two transition metals. We find that Ti remains in a higher formal valence (around 4+) independent of the Co concentration. In contrast to this, dramatic and systematic changes are observed for the Co as a function of y. We conclude that the stability of the Ti4+ triggers the A-site deficiency in our samples and predicts that oxygen vacancies are much more easily formed at large Co content, which in turn will greatly enhance the performance as electrode material.

Introduction

ABO3 perovskites with Ti in the B site are promising electrode materials for a new subtype of Solid Oxide Fuel Cells (SOFC), the so called Symmetrical SOFC (SSOFC), reported for first time by Ruiz-Morales et al. [1], [2]. SSOFC are based on a symmetric design where the same compound is used as cell anode and cathode. Advantages over traditional SOFC relies on their simpler design, dealing with compatibility and inter-diffusion problems between cell components and even helping to manage the anode sulfur and carbon poisoning by simply reversing the gas flux, issues that strongly affects SOFC anodes long term efficiency.

Perovskites belonging to the LaxSr1−xTiO3 (LST) family are recognized for their good properties in a SOFC anode reductive environment [3]. Besides, the replacement of small amounts of Ti with other transition metals can enhance their ionic and electronic conductivity in oxidizing atmospheres, therefore, enabling the use of doped LST as possible SOFC cathodes [4], [5]. Attending the wide experience gained with the La1−xSrxCoO3−δ (LSC) as mixed conductor for SOFC cathodes [6], [7] and the support of theoretical calculations [8], the substitution of Ti by Co atoms seems to be an adequate way to enhance LST mixed conductivity.

However, substitution of atoms with other valences in the ABO3 structure might induce oxidation and reduction processes in the components or even creation of vacancies in the oxygen or the A-site sublattice, in order to compensate for charge and size changes [9]. Some authors reported that doping SrTiO3 with 3+ ions on the perovskite A-site may increase the oxygen non-stoichiometry, creates A-site deficiency and/or changes the ratio of Ti4+ to Ti3+ thus enhancing the conductivity. The predominance of one of these compensating mechanisms depends on synthesis temperature and reducing conditions [3], [10]. The already mentioned replacement of Ti4+ on the perovskite B-site can also alter the structural properties of the titanates [11], [12]. Therefore, substitutions may not only affect the electrochemical behavior, but also the material structure itself. An important requirement in the optimization of doped titanates as SSOFC electrodes is to identify and understand the active charge compensation mechanisms and their influence over structural parameters and electronic configuration. For example: A-site deficiency is related to phase stability [10] and to mixed conductivity [13], O vacancies strongly influences ionic conductivity [6] and the transition metal (TM) oxidation state affects the electronic conductivity [11].

In a previous work we investigated the series LaxSr1−xTi1−yCoyOδ (LSTC) with x = 0.4 and y varying between 0.0 and 0.5 [14]. A structural characterization using high resolution synchrotron X-ray Powder Diffractometry (XPD) and Transmission Electron Microscopy (TEM) methods showed that the creation of Sr vacancies at the A-site is the main compensation mechanism for charge and size changes, and that the A-site vacancies concentration decreases with the incorporation of Co in the crystal structure. The existence of Sr segregation in samples with A-site deficiency was supported by the presence of an amorphous background in the XPD data and local crystallinity loss observed by TEM. The physical reason for the creation of A-site vacancies, however, remained to be clarified. Simultaneously, the characterization of La0.5Sr0.5Ti0.5Co0.5O3−δ through neutron diffraction measurements was reported [15], indicating that this compound is fully stoichiometric at room temperature and presented a different space group than our samples (i.e., for y = 0.5 and x = 0.5, this work reported a crystal structure corresponding to the orthorhombic Pbnm space group, while for a similar composition, y = 0.5 and x = 0.4, our best fit of XPD data was obtained assuming the R-3c rhombohedral space group).

We concluded from our previous studies that the presence of Co, which should modify its oxidation state more easily than Ti, might preclude the formation of A-site vacancies, even at low synthesis temperature. However, the lack of published data on the electronic properties of the B-site transition metals in this series made it impossible to validate that assumption. Moreover, the knowledge of the electronic configuration of the B-sites is crucial in order to understand the electrochemical properties of SSOFC electrodes.

In this work, we experimentally investigate the electronic configuration, oxidation state and nearest neighbors coordination behavior of cobalt and titanium in the same samples and tested our previous hypothesis using synchrotron X-ray Absorption techniques. These results will help to establish and characterize the LSTC charge compensation mechanisms and understand the physical origin of the electrochemical properties of these materials as SOFC electrode.

Section snippets

Samples and synthesis method

Samples with nominal compositions of La0.4Sr0.6Ti1−yCoyOδ with 0 ≤ y ≤ 0.5 (LSTC) were prepared by a citrate chemical route. Ti(IV)-butoxide, La2O3, SrCO3, and Co(NO3)2 were used as precursor materials; they were mixed in different ratios to get the desired compositions and the formed sol–gel was then calcinated at 300 °C. More details about this synthesis are reported elsewhere [14]. The as-prepared powders were sintered at 750 °C and at 1100 °C (Table 1) with grain sizes of about 40 and

Theory

The main purpose of the density functional theory (DFT) calculations performed in this study is to estimate the effects of purely structural changes on the Co K-edge XANES. To achieve this, the calculations were done for stoichiometric LaCoO3, using the structural data determined experimentally for our La0.4Sr0.6Ti1−yCoyOδ (y = 0.1, 0.3, 0.5) samples [14]. In addition we also performed a calculation for structure with the lattice constants for y = 0.1 expanded by 2%. The DFT calculations were

XANES (X-ray near edge structure)

The absorption coefficient at the cobalt K-edge of the LSTC samples and the reference materials are shown in Fig. 1A. The main absorption jump can be observed in all cobalt spectra between 7705 and 7725 eV. This peak is known as the “white line” (WL) and is due to strong 1s → 4p electric dipole transitions. In the following we will also define the edge position E0 as the first peak in the first derivative of the XANES spectra (the point with the steepest slope). Regarding the LSTC series, two

Discussion

As mentioned in the introduction, there are three mechanisms which are discussed in the literature in relation to the compensation of charge and size changes with doping in LSTC: (i) vacancies in the perovskite A-site, (ii) changes of the oxidation state of the perovskite B-site, or (iii) changes in the oxygen stoichiometry (usually through creation of oxygen vacancies).

Which of these mechanisms is active at least partially depends on the external conditions. For example, in LST materials

Conclusions

Our results show that in the La0.4Sr0.6Ti1−yCoyOδ materials the formal valence of Ti stays close to 4+ for all compositions, whereas the local atomic and electronic structures around Co change dramatically as a function of y. According to our DFT calculations, the structural changes around Co deduced from the EXAFS data have a very strong effect on the Co K-edge. The direct determination of the Co valence from the Co K-edge position is therefore not possible in the present case. However, the

Acknowledgements

This work has been supported by: the Brazilian Synchrotron Light Laboratory (LNLS) under proposals D04B – XAFS 11743 and XAFS1 – 12800, the Argentinean projects PICT-PAE 2288 and the PRH074 ANPCyT-CONICET and the BMBF-MinCyT binational cooperation agreement AL-10-10. CNEA is gratefully acknowledged for supplying equipment, technical staff and laboratories.

References (38)

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