High-temperature polaronic transport in PrBaCoTa(Nb)O6 perovskite-like phases

https://doi.org/10.1016/j.jpcs.2020.109645Get rights and content

Highlights

  • Electrical conductivity in Ta and Nb-doped cobaltite PrBaCo2O6–δ was measured.

  • Theoretical model for electron transport was developed and validated.

  • Co ions spin distribution was shown to influence the electrical properties.

Abstract

The electrical transport properties of dense PrBaCoTaO6 and PrBaCoNbO6 polycrystalline phases are thoroughly studied. Both measured conductivity and thermopower temperature dependencies are consistent with p-type adiabatic small polaron hopping mechanism. Detailed analysis based on DFT calculations reveals Co t2g orbitals play crucial role in charge transfer process. The proposed theoretical transport model predicts most trivalent Co ions tend to acquire an intermediate spin state acting as self-trapped electron holes. Estimated carrier mobility and polaron jump frequency values for both studied compounds are found to be in a reasonable coincidence with previously obtained results.

Introduction

Despite numerous efforts undertaken the development of stable and efficient intermediate temperature solid oxide fuel cells (IT-SOFCs) still remains a desirable goal to achieve [[1], [2], [3], [4]]. In particular, optimal chemical composition for cathode materials wasn't found yet. Layered cobaltites with general formula AA’Co2O6 where A and A′ denote rare- and alkaline-earth elements, respectively, are often considered as perspective candidates for practical implementation in IT-SOFCs [[5], [6], [7]]. These materials are distinguished by very high mixed ionic/electronic conductivity values [[8], [9], [10], [11]] and fast oxygen exchange kinetics even at 900 K [12,13]. However, several drawbacks restrict their application potential, in particular, relatively fast degradation in CO2 containing atmospheres [14] and unacceptably high values of thermal expansion coefficient (TEC) leading to mechanical instabilities in high-temperature devices [11]. In this regard various modifying strategies were implemented in order to improve the overall cathode performance of cobaltites [[15], [16], [17], [18], [19]]

Recently, cobalt based electrodes with additions of niobium ant tantalum were developed [16,17,[20], [21], [22]]. The injections of 4d/5d elements in cobalt-containing matrix occurred to be an attractive doping strategy because such problems as TEC mismatch and cathodes’ degradation under CO2 ambient can be solved simultaneously without sufficient suppression of cathode functional properties. One should notice the nature of the resulting Nb/Ta-doped materials differs significantly depending on the total dopant concentration. The single phase samples from the solid solution PrBa1-xCo2-yTayO6-δ with 0.01≤y ≤ 0.05 were successfully synthesized [17]. On the other hand, electrochemical properties of the composite (1–x) PrBaCo2O6–δ – (x) PrBaCoNbO6 electrodes [20] where Nb-containing phase maintains ordered double perovskite structure were studied. The results obtained evidence these chemical compositions are promising cathode materials. However, numerous questions regarding the nature of PrBaCoNbO6 additive remain unclear, for example a mechanism of electrical conductivity, oxygen ion transfer and thermal expansion features.

In previous work [23] we've tried to answer these questions using a combination of theoretical and experimental approaches. It was shown PrBaCoNbO6 (PBCN) and PrBaCoTaO6 (PBCT) possess very small oxygen stoichiometry changes even at 1223 K thus excluding the possibility of their appreciable contribution to ionic transport in composite electrodes studied in Ref. [20]. Moreover, the respective TEC values appeared to be commensurate with those for common electrolytes. Calculated electron structure for both PBCN and PBCT revealed these materials are wide-gap semiconductors that is qualitatively confirmed by the results obtained in Ref. [20,24].

In this paper we continue to develop theoretical concepts underlying the functional properties observed for PBCN/PBCT phases, in particular, electron transport model is proposed and verified using experimental data.

Section snippets

Experimental

PrBaCoTa(Nb)O6 oxide samples were synthesized using conventional solid state route. High purity Pr6O11, BaCO3, Ta2O5, Nb2O5 and metallic Co were selected as starting reagents, weighted in proper amounts and thoroughly mixed in an agate mortar in ethanol media. Then the resulted powder was heated up to 1173 K in order to oxidize Co and remove CO2 with adsorbates. Further synthetic operations included pelletizing of the powders obtained and subsequent firing in 1400–1650 K temperature range. The

Results and discussion

X-Ray diffraction spectra for PrBaCoTa(Nb)O6 samples refined by Rietveld method are presented in Fig. 2. It can be seen the synthesized specimens are single-phase in accord with the previous results, the respectively determined space group (Fm-3m) and calculated unit cell parameters coincide with those presented earlier [23].

The SEM images of polished cross-sections of the PBCT and PBCN samples are shown in Fig. 3.

It can be seen the poreless ceramics was obtained having homogeneously

Conclusions

PrBaCoTa(Nb)O6 oxides with double perovskite structure were synthesized by means of conventional solid state reaction route, the obtained samples were confirmed to be single-phase. Sintered ceramic specimens were shown to possess pore-free polycrystalline microstructure. The electrical transport measurements revealed the studied compounds were characterized as wide-gap p-type semiconductors with adiabatic small polaron charge transfer mechanism. Ab initio calculations evidenced the valence band

CRediT authorship contribution statement

B.V. Politov: Conceptualization, Methodology, Formal analysis, Funding acquisition, Writing - original draft. E.A. Antipinskaya: Investigation, Data curation, Visualization. I.R. Shein: Software. A.Yu Suntsov: Conceptualization, Funding acquisition, Supervision, Writing - review & editing.

Declaration of competing interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

B.V. Politov appreciates the Russian Foundation for Basic Research under grant №18-33-01073. The authors are also thankful to government assignment № AAAA-A19-119110190048-7 for the support of this work. The DFT modeling was performed at the URAN cluster of the Institute of Mathematics and Mechanics belonging to the UB RAS.

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