Font Size: a A A

Effects Of A/B-site Substitutions On Structure,piezoelectric And Multiferroic Properties Of BiFeO3-BaTiO3-based Lead-free Ceramics

Posted on:2017-04-07Degree:MasterType:Thesis
Country:ChinaCandidate:L L LuoFull Text:PDF
GTID:2271330482497975Subject:Materials science
Abstract/Summary:PDF Full Text Request
Multiferroics refers to a kind of multifunctional material which exhibit both ferroelectric and ferromagnetic properties. As a rare single-phase multiferroic material at room temperature, Bi Fe O3 has been attracted much attention because it shows both ferroelectricity(TC = 830 °C) and G-type antiferromagnetism(TN = 370 °C). However,for pure Bi Fe O3 ceramics, there are some inherent impediments to its ferroelectricity,piezoelectricity and ferromagnetism. Besides, pure Bi Fe O3 usually possesses high leakage current because of the volatilization of Bi and reduction of Fe3+ to Fe2+ during sintering. To prevent the formation of impurities, improve resistivity and multiferroic of the Bi Fe O3 ceramics, A-site substitution or A, B-site co-substitution with ions(A-site substitution with La3+ 、 Sm3+ for Bi3+ and B-site substitution with(Mg0.5Zr0.5)3+,(Ni0.5Mn0.5)3+and(Co0.5Mn0.5)3+) were carried out. The main results are as follows:(1)(0.725-x)Bi Fe O3-x Bi(Mg0.5Zr0.5)O3-0.275 Ba Ti O3 + 1 mol% Mn O2 lead-free ceramics(x = 0-0.08) were synthesized by a conventional solid state reaction method and the effects of Bi(Mg0.5Zr0.5)O3 on phase transition, piezoelectric and ferroelectric properties of the ceramics were investigated. After the addition of Bi(Mg0.5Zr0.5)O3, the crystal structure of the ceramics is transformed from rhombohedral to tetragonal phase and the morphotropic phase boundary(MPB) of rhombohedral and tetragonal phase is formed at x = 0.01. The grain size of the ceramics increases with x increasing from 0 to0.02 and then decreases with x further increasing. The dielectric peak of the ceramics becomes diffusive with x increasing after the addition of Bi(Mg0.5Zr0.5)O3. The ceramics with x = 0-0.08 exhibit much better electric insulation with the resistivity of1.0×109-5.0×109 Ω·cm than pure Bi Fe O3 ceramic with the resistivity of 5×107 Ω·cm.Due to the formation of the MPB, the ceramics with x = 0-0.02 possess gooddensification with the relative densities ρr of 94.9-96.3 %, strong piezoelectricity with the d33 of 129-135 p C/N and very high Curie temperature with the TC of 559-610 °C.(2)(0.725-x)Bi Fe O3-x Bi(Ni0.5Mn0.5)O3-0.275 Ba Ti O3 + 1 mol% Mn O2 multiferroic ceramics were synthesized by a conventional solid state reaction method and the effects of Bi(Ni0.5Mn0.5)O3 on phase transition, piezoelectric and multiferroic properties of the ceramics were investigated. All the ceramics sintered at 950 o C for 2 h possess a pure perovskite structure. Rietveld refinement of X-ray diffraction data revealed that a coexistence of rhombohedral and pseudocubic phases are formed at x =0.05-0.07. After the addition of Bi(Ni0.5Mn0.5)O3, the grain growth is suppressed because of the diffusion of Mn4+into the grain boundary. The dielectric peak becomes gradually diffusive with increasing x due to the small difference between Fe3+ and(Ni0.5Mn0.5)3+. After the addition of a small amount of Bi(Ni0.5Mn0.5)O3(x £ 0.02), the ceramics possess strong piezoelectricity with d33 of 124-145 p C/N, strong ferroelectric with Pr of 16.7-19.3 μC/cm2 and ME coefficient performance with α33 of 553.65 m V cm-1 Oe-1.(3)(0.75-x)Bi Fe O3-0.25 Ba Ti O3-x La(Co0.5Mn0.5)O3 + 1 mol% Mn O2 lead-free ceramics(x = 0-0.10) were synthesized using conventional solid-state reaction route and the effects of La(Co0.5Mn0.5)O3 on phase transition, piezoelectric, ferroelectric and multiferroic properties of the ceramics were investigated. After the addition of La(Co0.5Mn0.5)O3, the crystal structure of the ceramics is transformed from rhombohedral(space group R3c) to orthorhombic symmetry(space group Amm2), and the morphotropic phase boundary(MPB) of rhombohedral and orthorhombic phase is formed at x = 0.01-0.03. The dielectric peak of the ceramics was found to become diffusive with increasing x. The ceramics with x = 0-0.03 possess strong piezoelectricity with d33 of 95–108 p C/N, strong ferroelectricity with Pr of 2.2-18.1μC/cm2, considerable magnetoelectric coefficient of 372-672 m V/cm·Oe, and high Curie temperature of 523-659 °C.(4)(0.75-x)Bi Fe O3-0.25 Ba Ti O3-x Sm Co O3 + 1 mol% Mn O2 lead-free multiferroic ceramics were synthesized using a conventional solid-state reaction route. The effect of Sm Co O3 on phase structure, piezoelectricity and multiferroicity of the ceramics were investigated. The crystalline structure of the ceramics is transformed from rhombohedral to tetragonal symmetry with increasing the amount of Sm Co O3. A morphotropic phase boundary of rhombohedral and tetragonal phases is formed at x =0.01-0.04. A small doping amount of Sm Co O3 is shown to improve the ferroelectric,piezoelectric and magnetoelectric properties of the ceramics. For the ceramics with x =0.01-0.03, high resistivity, piezoelectricity and ferroelectricity are obtained. The ferromagnetism of the materials is greatly enhanced by the doping of Sm Co O3 such that a very high magnetoelectric coefficient of 742 m V/cm·Oe is obtained at x = 0.01.
Keywords/Search Tags:BiFeO3-BaTiO3, Perovskite, multiferroic, Ferroelectric and piezoelectric properties, magnetoelectric coupling
PDF Full Text Request
Related items