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Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic
Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic
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Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic
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Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic
Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic

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Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic
Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic
Journal Article

Modified crystal structure, dielectric properties, and magnetic phase transition temperature of Ca doped BiFeO3 ceramic

2018
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Overview
This paper deals with the preparation of multiferroic Bi 1− x Ca x FeO 3 ( x  = 0–0.2) ceramics with the sol–gel method and a study on the influence of Ca 2+ doping on the structure, dielectric, and ferromagnetic properties of BiFeO 3 ceramics. The result shows that the XRD analysis reveals a phase transition in Ca-doped BiFeO 3 from rhombohedral to orthorhombic when x is greater than 0.1. The dielectric constant ( ε r ) of Bi 0.9 Ca 0.1 FeO 3 measured at 1 kHz is about seven times greater than that of BiFeO 3 , and Bi 0.8 Ca 0.2 FeO 3 is less than one-tenth of BiFeO 3 . It might be understood in terms of the dipole polarization, oxygen vacancy and lattice phase transition. Magnetic measurements show that the M-H of Bi 1 − x Ca x FeO 3 samples exhibit unsaturated and symmetric magnetic hysteresis loops with the increase of Ca 2+ , indicating the weakly ferromagnetic behavior. It indicates that there is coexistence of Fe 2+ and Fe 3+ in Bi 1 − x Ca x FeO 3 samples according to the XPS spectrum. The ratio of Fe 2+ /Fe 3+ increases with doping Ca 2+ content and the magnetic properties of BiFeO 3 are enhanced. It is evident that the ferromagnetic phase transition of BiFeO 3 samples occurs at 878 K by measuring the M–T and DSC curves. The T N of BiFeO 3 will be reduced from 644 to 638 K and the T M does not change slightly at 878 K with increasing Ca 2+ content. T N and T M of Bi 1 − x Ca x FeO 3 change depends mainly on the magnetic structure of relative stability and Fe–O–Fe super-exchange strength. Graphical abstract The grains of BiFeO 3 sample appear cube shaped, while more irregular grains of Bi 1 − x Ca x FeO 3 sample are formed with doping Ca 2+ from Fig. 2. M-H of BiFeO 3 exhibit saturated and symmetric magnetic hysteresis loops at room temperature with doping Ca 2+ , indicating that Ca 2+ doping can improve the ferromagnetic properties of BiFeO 3 . It is evident that the ferromagnetic phase transition of Bi 1- x Ca x FeO 3 samples occurs at 878K by measuring the M-T and DSC curves.