Compositional induced structural phase transitions in (1 − x)(K0.5Na0.5)NbO3–x(Ba0.5Sr0.5)TiO3 ferroelectric solid solutions

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作者
Satyaranjan Sahoo
Dhiren K. Pradhan
Shalini Kumari
Koyal Suman Samantaray
Charanjeet Singh
Anupam Mishra
Md. Mijanur Rahaman
Banarji Behera
Ashok Kumar
Reji Thomas
Philip D. Rack
Dillip K. Pradhan
机构
[1] National Institute of Technology Rourkela,Department of Physics and Astronomy
[2] University of Tennessee,Department of Materials Science and Engineering
[3] The Pennsylvania State University,Department of Materials Science & Engineering
[4] Indian Institute of Technology Indore,Department of Physics
[5] CSIR-National Physical Laboratory,Department of Materials Engineering
[6] Academy of Scientific and Innovative Research (AcSIR),Department of Materials Science and Engineering
[7] Indian Institute of Science,School of Physics
[8] University of Rajshahi,Division of Research and Development
[9] Sambalpur University,School of Chemical Engineering and Physical Sciences
[10] Lovely Professional University,undefined
[11] Lovely Professional University,undefined
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摘要
Ferroelectric materials exhibiting switchable and spontaneous polarization have strong potential to be utilized in various novel electronic devices. Solid solutions of different perovskite structures induce the coexistence of various phases and enhance the physical functionalities around the phase coexistence region. The construction of phase diagrams is important as they describe the material properties, which are linked to the underpinning physics determining the system. Here we present the phase diagram of (K0.5Na0.5NbO3)–(Ba0.5Sr0.5TiO3) (KNN-BST) system as a function of composition and their associated physical properties. Lead-free (1 − x)KNN–xBST (0 ≤ x ≤ 0.3) solid solution ceramics were synthesized by conventional solid-state reaction technique. The X-ray diffraction and Raman spectroscopic studies indicate composition-dependent structural phase transitions from an orthorhombic phase for x = 0 to orthorhombic + tetragonal dual-phase (for 0.025 ≤ x ≤ 0.15), then a tetragonal + cubic dual-phase (x = 0.2) and finally a cubic single phase for x ≥ 0.25 at room temperature (RT). Among these, the orthorhombic + tetragonal dual-phase system shows an enhanced value of the dielectric constant at room temperature. The phase transition temperatures, orthorhombic to tetragonal (TO-T) and tetragonal to cubic (TC), decrease with the increase in BST concentrations. The ferroelectric studies show a decrease of both 2Pr and EC values with a rise in BST concentration and x = 0.025 showed a maximum piezoelectric coefficient.
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