Ferroelectric properties of (1 − x)Bi(Zn1/2Ti1/2)O3–xPbZrO3 ceramics

The (1 − x)Bi(Zn1/2Ti1/2)O3–xPbZrO3 solid solution ceramics were prepared by using solid-state reaction method, and their ferroelectric properties were investigated. It was found that the perovskite structure is stable for compositions with x ≥ 0.900. Within this composition range, the crystal structure of the solid solution preserves the orthorhombic symmetry of PbZrO3 (PZ). The Curie point of the ceramics was found to decrease with increasing Bi(Zn1/2Ti1/2)O3 (BZT) content. The intermediate ferroelectric phase of PZ was stabilized by BZT addition and exists within a much wider temperature range in the solid solution

The Morphotropic Phase Boundary in the (1-x)PbZrO3–x[0.3Bi(Zn1/2Ti1/2)O3–0.7PbTiO3] Perovskite Solid Solution

Ceramics in the (1-x)PbZrO3–x[0.3Bi(Zn1/2Ti1/2)O3–0.7PbTiO3] solid solution system with 0.48 x 0.56 were investigated. A morphotropic phase boundary separating rhombohedral and tetragonal perovskite phases was identified at x = 0.52. This composition displays the maximum remanent polarization Pr of 40.7 μC/cm2 and the best piezoelectric coefficient d33 of 311 pC/N in the pseudo-binary system. However, the Curie temperature Tc for this MPB composition is 291 °C, much lower than initially expected

The morphotropic phase boundary and electrical properties of (1 − x)Pb(Zn1/2W1/2)O3–xPb(Zr0.5Ti0.5)O3 ceramics

Ceramics in the solid solution of (1 − x)Pb(Zn1/2W1/2)O3–xPb(Zr0.5Ti0.5)O3 system, with x = 0.80, 0.85, 0.90, and 0.95, were synthesized with the solid-state reaction technique. The perovskite phase formation in the sintered ceramics was analyzed with X-ray diffraction. It shows that the rhombohedral and the tetragonal phases coexist in the ceramic with x = 0.90, indicating the morphotropic phase boundary (MPB) within this pseudo-binary system. Dielectric and ferroelectric properties measurements indicate that the transition temperature decreases while the remanent polarization increases with the addition of Pb(Zn1/2W1/2)O3. In the composition of x = 0.85 which is close to the MPB in the rhombohedral side, a high piezoelectric property with d 33 = 222 pC/N was observed

Cation, dipole, and spin order in Pb(Fe2/3W1/3)O3-based magnetoelectric multiferroic compounds

Long range 1:1 cation order was developed in Pb(Fe2(1−x)/3Sc2x/3W1/3)O3solid solution compounds by high temperature solid state reaction. It is found that the degree of cation order directly influences the saturation magnetization in these single phase compounds. A high saturation magnetization (∼0.61μB/f.u.) was observed for x=0.15 at 10Kunder 5T. A ferrimagnetic structure was suggested to take into account for the observed magnetic behavior. These compounds also display a saturated electrical polarization of ∼15μC/cm2 at 40kV/cm at 120K

Identification of Barium-Site Substitution of BiFeO3-Bi0.5K0.5TiO3 Multiferroic Ceramics: X-ray Absorption Near Edge Spectroscopy

In this work, the effects of barium substitution on the local structure, dielectric and magnetic properties of the polycrystalline ceramics 0.6BiFeO3–0.4(Bi0.5K0.5)TiO3 (0.6BFO–0.4BKT) system was investigated. A solid-state reaction technique was used to synthesize the materials with barium (Ba) doping of 1, 3, 5, 7, and 10 mol%. XRD analysis reveals the coexistence between tetragonal and rhombohedral phases of single-phase perovskite in pure 0.6BFO–0.4BKT and the rhombohedral reach phase was found with increasing Ba content. XANES simulations indicate that the majority of Ba atoms occupy A-site in BKT lattice of Ba-doped 0.6BFO-0.4BKT, the oxidation state of Fe, Ti, and Ba ions are +3, +4 and +2, respectively. At 5 mol% of Ba doping content, the dielectric measurement shows the morphotropic phase boundary (MPB) and the maximum value of ferromagnetic characteristic were observed, indicating an optimum composition, properties and production conditions

Dielectric, ferroelectric and piezoelectric properties of13; (1 x2013; x)[Pb0.91La0.09(Zr0.60Ti0.40)O3]x2013;x[Pb(Mg1/3Nb2/3)O3],13; 0 xA3; x xA3; 1

The dielectric, ferroelectric, and piezoelectric13; properties of ceramic materials of compositions13; (1 x2013; x)[Pb0.91La0.09(Zr0.60Ti0.40)O3]x2013;x[Pb(Mg1/3Nb2/3)O3],13; x = (0, 0.2, 0.4, 0.6, 0.8, and 1.0) were studied. The above13; compositions were prepared by mixing the individual13; Pb0.91La0.09(Zr0.60Ti0.40)O3 (PLZT) and Pb(Mg1/3Nb2/3)13; O3 (PMN) powders in order to design materials with13; different combination of piezo and dielectric properties.13; The powders were calcined at 850 C for 4 h. The presence13; of various phases in the calcined powders was13; characterized by X-ray diffraction (XRD) technique.13; The compacts were prepared by uniaxial pressing and13; were sintered at 1250 C for 2 h. The sintered compacts13; were electroded, poled at 2 kV/mm dc voltage and their13; dielectric, ferroelectric, and piezoelectric properties13; were measured. In general, it was observed that the13; dielectric constant, loss factor and the slimness of the13; ferroelectric curves increase with the PMN content13; while the remnant polarization, saturation polarization,13; and the coercive fields were decreased. It is now possible13; to design materials with a wide combination of d33, K,13; and loss factor by varying PLZT and PMN ratio