Improved ferroelectric and pyroelectric properties of Pb-doped SrBi4Ti4O15 ceramics for high temperature applications
Graphical abstract
Introduction
The bismuth layer structured ferroelectric (BLSF) materials, due to their fatigue-free properties, have received significant attention for their application in non-volatile ferroelectric random access memory [1], [2], [3]. Compounds of this class possess relatively low-loss, low dielectric constant, higher resistance to aging and strong anisotropic electromechanical factors. In addition, these materials have higher ferroelectric ordering temperature and low temperature coefficient of resonance frequency, making them attractive for high temperature pyro- and piezoelectric applications [4], [5].
These compounds have pseudo-perovskite (Am−1BmO3m+1)2− blocks interleaved with an insulating (Bi2O2)2+ layers along the c-axis. In this formula, A represents mono-, di- and trivalent ions, or a mixture of them, B represents tetra-, penta- or hexavalent ions and m (=1, 2, 3…) is the BO6 octahedra in the pseudo-perovskite block. The spontaneous polarization of BLSF arises from different modes of simultaneous rotation of oxygen octahedra. The displacements of ions in the perovskite B-sites contribute a major component of polarization in the a–b plane of the pseudo-perovskite layers. Among the BLSF compounds SrBi2Ta2O9, Bi3.25La0.75Ti3O12 and SrBi4Ti4O15 are the most promising candidates due to their good ferroelectric polarization and fatigue resistance up to 1012 cycles [1], [3]. The fatigue-free property of these oxides is believed to originate from the insulating role of Bi2O2 layers as they are considered to be the compensation of space charges built-up near the electrode and/or suppression of ionic diffusion [6], [7]. In addition, these materials are believed to be chemically more stable structure than volatile Pb-containing oxides. The present work investigates the ferroelectric properties of modified SrBi4Ti4O15 (SBT) ceramics.
SBT with m = 4 is a typical material that has been studied by many researchers for its piezoelectric and pyroelectric applications [8], [9], [10], [11], [12]. It crystallizes in orthorhombic structure with a space group A21am and has a b/a ratio of less than 1. The effect of doping at A- and B-sites of the lattice has shown some interesting changes on ferroelectric and pyroelectric properties of SBT. Zhao et al. [4] showed improved ferroelectric and pyroelectric properties in A- and B-site modified SBT ceramics. Similarly, Hirose et al. [10] showed that the La-modification in SBT ceramics resulted in the enhanced mechanical quality factor (Qm) of 69.6, which is larger than that obtained for PbTiO3 (19.1) ceramics. Recently, Rout et al. [12] synthesized fine grained SBT ceramics using the soft chemical method and studied the contribution of bulk and grain boundaries on electrical properties using impedance spectroscopy. In our earlier work, we reported interesting structural and magnetic properties of (Bi, La)FeO3 modified SBT [13]. In the present work, we modified SBT with Pb (doping concentration up to 40 mol.%) to study the changes in its phase transitions and ferroelectric properties. It was shown that PbBi4Ti4O15 (PBT), in spite of the presence of lead at A-site do not show any degradation in polarization even up to 1010 cycles [14]. Hence, it will be interesting to study the effect of chemically induced strain on its structure and physical properties, particularly the polarization. In order to avoid the volatility of Pb and Bi of the resulting compositions, the materials were synthesized via the modified sol–gel combustion method.
We observed an improved ferroelectric and pyroelectric properties in these ceramics along with an improved d33∼22 pC/N for 40 mol.% Pb-doped SBT, against 18 pC/N for undoped SBT ceramics.
Section snippets
Experimental
Ceramic samples of Sr1−xPbxBi4Ti4O15 with x = 0.0 (SBT), 0.1 (SPBT1), 0.2 (SPBT2), 0.3 (SPBT3) and 0.4 (SPBT4) were synthesized by modified sol–gel method. Starting raw materials for the synthesis were: high purity (Aldrich, 99.9%) strontium nitrate [Sr(NO3)2], bismuth nitrate pentahydrate [Bi(NO3)3·5H2O], lead acetate and titanium dioxide [TiO2, particle size < 50 nm]. Stoichiometric amounts of above nitrates were mixed in solution and TiO2 was added to it, followed by stirring to yield an aqueous
Results and discussion
The X-ray patterns of the final sintered samples are shown in Fig. 1. All the peaks were indexed based on the reported data of SBT ceramics indicating the formation of single-phase compounds of Aurivillius phases with space group A21am [17], [18]. Some variations observed in the intensities and peak positions in XRD patterns can be attributed to the variations in lattice distortions of the samples. The lattice parameters calculated using the CHEKCELL program for SBT are a = 5.4505, b = 5.4391 and c =
Conclusion
4-layered SBT ceramics with Pb-modification were synthesized to study the effect of Pb modification on ferroelectric and pyroelectric properties. The change in chemical composition transformed the crystal structure and resulted in a higher tetragonal strain, which influenced the phase transitions. From the complex impedance spectroscopy it was observed that the Pb-doping has resulted in the improved grain boundary resistivity. The modification resulted in the improved pyroelectric activity with
Acknowledgements
The authors would like to acknowledge the financial support from FCT, Portugal (SFRH/BPD/75582/2010).
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