Polycrystalline BiFe1-xScxO3 (x=0, 0.05, 0.1 and 0.15) compounds are prepared using solid state reaction. The XRD patterns show that all compounds are crystallized in rhombohedral structure with R3c space group. An induced weak ferromagnetism in Sc substituted BiFeO 3 due to suppression of spiral modulated spin structure is revealed. In addition, a spin glass like behaviour is observed from the zero field cooled (ZFC) and field cooled (FC) magnetization curves in the low temperature region. Further, the coupling between the ferroelectric and (anti) ferromagnetic orders is evident from the appearance of anomaly in the dielectric data near the magnetic Néel temperature (373 °C). The reduction of oxygen vacancies due to Sc substitution is evid...
The weak and deficient manipulation of charge-spin coupling in multiferroic BiFeO3 (BFO) notoriously...
AbstractMultiferroics exhibit unique combination of ferroic properties, simultaneously. For instance...
10.1016/j.jmmm.2008.04.119Journal of Magnetism and Magnetic Materials320182215-2220JMMM
Polycrystalline BiFe1-xScxO3 (x=0, 0.05, 0.1 and 0.15) compounds are prepared using solid state reac...
Polycrystalline BiFeO3 and Bi0.9Nd0.1Fe1- xScxO3 (x = 0, 0.05, and 0.10) multiferroic compounds were...
BiFeO3 (BFO) and Bi0.85Sm0.15Fe0.90Sc0.10O3 (BSFSO) ceramics were synthesized by conventional solid ...
Polycrystalline BiFeO3 and Bi0.9Nd0.1Fe1- xScxO3 (x = 0, 0.05, and 0.10) multiferroic compounds were...
The polycrystalline Bi1-xEuxFeO 3 (x=0, 0.05, and 0.1) ceramics were synthesized by conventional sol...
BiFeO 3 (BFO) is well known room temperature multiferroic among all perovskite kind multiferroics....
Abstract Polycrystalline BiFe1-xScxO3 (x = 0, 0.05, 0.10 and 0.15) compounds were prepared using sol...
The polycrystalline Bi 1-xHo xFeO 3 (x=0, 0.05, 0.1) compounds were synthesized by conventional soli...
The polycrystalline Bi1-xEuxFeO 3 (x=0, 0.05, and 0.1) ceramics were synthesized by conventional sol...
Polycrystalline BiFeO3 and rare earth substituted Bi 0.9R0.1FeO3 (BRFO, R=Y, Ho and Er) compounds we...
Structural, magnetic, and electrical properties of polycrystalline Y-Sc codoped BiFeO3 (BFO) ceramic...
"Conventional solid state reaction method, from oxides and carbonates, was employed to prepare bismu...
The weak and deficient manipulation of charge-spin coupling in multiferroic BiFeO3 (BFO) notoriously...
AbstractMultiferroics exhibit unique combination of ferroic properties, simultaneously. For instance...
10.1016/j.jmmm.2008.04.119Journal of Magnetism and Magnetic Materials320182215-2220JMMM
Polycrystalline BiFe1-xScxO3 (x=0, 0.05, 0.1 and 0.15) compounds are prepared using solid state reac...
Polycrystalline BiFeO3 and Bi0.9Nd0.1Fe1- xScxO3 (x = 0, 0.05, and 0.10) multiferroic compounds were...
BiFeO3 (BFO) and Bi0.85Sm0.15Fe0.90Sc0.10O3 (BSFSO) ceramics were synthesized by conventional solid ...
Polycrystalline BiFeO3 and Bi0.9Nd0.1Fe1- xScxO3 (x = 0, 0.05, and 0.10) multiferroic compounds were...
The polycrystalline Bi1-xEuxFeO 3 (x=0, 0.05, and 0.1) ceramics were synthesized by conventional sol...
BiFeO 3 (BFO) is well known room temperature multiferroic among all perovskite kind multiferroics....
Abstract Polycrystalline BiFe1-xScxO3 (x = 0, 0.05, 0.10 and 0.15) compounds were prepared using sol...
The polycrystalline Bi 1-xHo xFeO 3 (x=0, 0.05, 0.1) compounds were synthesized by conventional soli...
The polycrystalline Bi1-xEuxFeO 3 (x=0, 0.05, and 0.1) ceramics were synthesized by conventional sol...
Polycrystalline BiFeO3 and rare earth substituted Bi 0.9R0.1FeO3 (BRFO, R=Y, Ho and Er) compounds we...
Structural, magnetic, and electrical properties of polycrystalline Y-Sc codoped BiFeO3 (BFO) ceramic...
"Conventional solid state reaction method, from oxides and carbonates, was employed to prepare bismu...
The weak and deficient manipulation of charge-spin coupling in multiferroic BiFeO3 (BFO) notoriously...
AbstractMultiferroics exhibit unique combination of ferroic properties, simultaneously. For instance...
10.1016/j.jmmm.2008.04.119Journal of Magnetism and Magnetic Materials320182215-2220JMMM