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Soft Modes and Local Structural Transitions in Pb-free Ba(Ti0.8Zr0.2)O3-x(Ba0.7Ca0.3)TiO3 (x = 0.5): Pressure- and Temperature-dependent Raman Studies

TLDR
In this article, the Raman studies of a new lead-free relaxor ferroelectrics, Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCTZO), are compared with the eigenmodes of BTO calculated by using an ab-initio quantum-mechanical frozen-phonon method.
Abstract
We report our Raman studies of a new lead-free relaxor ferroelectrics, Ba0.85Ca0.15Ti0.9Zr0.1O3 (BCTZO). The Raman modes of BCTZO are compared with those of BaTi0.8Zr0.2O3 (BTZO), and BaTiO3 (BTO). Also, they are compared with the eigenmodes of BTO calculated by using an ab-initio quantum-mechanical frozen-phonon method. The sharp mode at 321 cm-1 of BTO, reported as a coupled mode showing an interference effect, becomes progressively broader in BTZO and BCTZO. This behavior, together with a broadening of the 527-cm-1 mode, suggests that the mode-coupling is weakened in BTZO and BCTZO. The structural transitions of BCTZO were investigated as functions of pressure at pressures below 20 GPa and of temperature at temperatures below 600 K. Three characteristic pressure-induced transitions, on each at 2.5, 5.0, and 13.0 GPa, were found. The transitions are suggested by the drastic changes in phonon modes (two softening modes, one each at ~ 300 and ~ 530 cm-1) and by the transformation of the intensity profile. A temperature-induced transition was found at a Curie temperature of ~ 380 K, where the average structure changes from tetragonal to cubic. It is accompanied by a softening mode at ~ 530 cm-1. The phonon spectrum of BCTZO suggests that its local environment is close to that of BTZO. However, the characteristic pressures of BCTZO are close to those of BTO. The sequence of pressure-induced transitions in both BCTZO and BTZO illustrate rich interplay between the long-range averaged structure and the short-range local order such that four distinguishable phases are suggested: tetragonal, locally ordered but compensated cubic, disordered cubic, and ideal cubic. We found that the critical pressures are plausibly related to the average crystal lattice.

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Journal ArticleDOI

Single-crystal high entropy perovskite oxide epitaxial films

TL;DR: In this article, a single-crystal epitaxial thin films of a high entropy perovskite oxide are synthesized using Pulsed laser deposition to grow the configurationally disordered $AB{\mathrm{O}}_{3}$ pervskite on MgO substrates.
Journal ArticleDOI

Single Crystal High Entropy Perovskite Oxide Epitaxial Films

TL;DR: In this paper, the first examples of single crystal epitaxial thin films of a high entropy perovskite oxide are synthesized using Pulsed Laser Deposition (PLD) and X-ray diffraction and scanning transmission electron microscopy demonstrate that the films are single phase with excellent crystallinity and atomically abrupt interfaces to the underlying substrates.
Journal ArticleDOI

Effects of Bi2O3 additive on sintering process and dielectric,ferroelectric, and piezoelectric properties of (Ba0.85Ca0.15)(Zr0.1Ti0.9)O3 lead-free piezoceramics

TL;DR: In this paper, the microstructure, phase composition, and local structure were investigated by scanning electron microscopy, X-ray diffraction, and Raman spectroscopy, and the incorporation of Bi3+ into the B-site of the perovskite BCZT structure.
Journal ArticleDOI

B-site modified photoferroic Cr3+-doped barium titanate nanoparticles: microwave-assisted hydrothermal synthesis, photocatalytic and electrochemical properties

TL;DR: In this paper, the photoferroic Cr3+-doped BaTiO3 nanoparticles with nominal Cr content ranging from 2-8 mol% were synthesized by a microwave-assisted hydrothermal method.
Journal ArticleDOI

Electromechanical properties of Ce-doped (Ba0.85Ca0.15)(Zr0.1Ti0.9)O3 lead-free piezoceramics

TL;DR: In this article, an approach for reducing the sintering temperature and increasing the electromechanical strain response of (Ba, Ca, Zr, Ti)O3 piezoceramics by aliovalent doping with Ce is presented.
References
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Journal ArticleDOI

Electromechanical Properties of Relaxor Ferroelectric Lead Magnesium Niobate-Lead Titanate Ceramics

TL;DR: The results of a recent investigation of the dependence of induced piezoelectric activity on temperature, electric bias field, and frequency and the electrostrictive response in the relaxor ferroelectric lead magnesium niobate-lead titanate ceramics (Pb(Mg1/3Nb2/3)O3)- x(PbTiO3)) at compositions below 30% PT are presented in this article.
Journal ArticleDOI

Effect of high pressure on relaxor ferroelectrics

TL;DR: In this paper, a high-pressure investigation by Raman spectroscopy of a relaxor ferroelectric (relaxor) was carried out and the results showed that an external pressure of several GPa, as can be met in thin films, alters fundamentally the structural and polar properties of PMN, suggesting that intrinsic instabilities towards pressure play an important role in the reduction of dielectric properties.
Journal ArticleDOI

Local structure in BaTi 1 − x Zr x O 3 relaxors from neutron pair distribution function analysis

TL;DR: The pair distribution functions (PDF) of the BTZ relaxors were determined at 300 K from neutron powder scattering data in this article, and it was shown that the Ti and Zr atoms do not occupy the equivalent octahedral sites expected from the crystallographic cubic perovskite structure.
Journal ArticleDOI

Pressure-induced disappearance of the local rhombohedral distortion in BaTiO3

TL;DR: In this paper, BaTiO3 has been studied by X-ray absorption spectroscopy at the Ti K edge up to 19 GPa in a diamond anvil cell at room temperature, where the intensity of the pre-edge features decreases indicating that the Ti atom is moving toward the centre of the oxygen octahedron.
Journal ArticleDOI

Phonon interference in BaTiO3: High-pressure Raman study.

TL;DR: Raman experiments have been carried out on single crystals of BaTiO 3 as a function of pressure up to 3.5 GPa across the ferroelectric to paraelectric phase transition to obtain pressure dependence of the line shape parameters and the coupling constants.
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