Acta Metallurgica Sinica (English Letters) ›› 2016, Vol. 29 ›› Issue (6): 505-517.DOI: 10.1007/s40195-016-0408-z
• Orginal Article • Next Articles
M. J. Miah1,2(
), A. K. M. Akther Hossain1
Received:2016-03-28
Revised:2016-03-28
Online:2016-03-28
Published:2016-06-10
M. J. Miah, A. K. M. Akther Hossain. Magnetic, Dielectric and Complex Impedance Properties of xBa0.95Sr0.05TiO3-(1 - x)BiFe0.9Gd0.1O3Multiferroic Ceramics[J]. Acta Metallurgica Sinica (English Letters), 2016, 29(6): 505-517.
| x | a (Å) | c (Å) | V (Å3) | ρB (g/cm3) | ρth (g/cm3) | t | P (%) | D (μm) |
|---|---|---|---|---|---|---|---|---|
| 0.00 | 5.5457 | 13.7038 | 367 | 7.60 | 8.83 | 0.847 | 13.9 | 2.17 |
| 0.10 | 5.5790 | 13.6028 | 368 | 7.38 | 8.54 | 0.855 | 13.5 | 2.60 |
| 0.20 | 5.5859 | 13.5698 | 368 | 7.10 | 8.28 | 0.864 | 13.0 | 2.47 |
| 0.25 | 5.6001 | 13.7960 | 374 | 7.06 | 8.03 | 0.868 | 12.0 | 2.42 |
Table 1 Lattice parameters, unit cell volume (V), bulk density (ρB), theoretical density (ρth), tolerance factor (t), porosity (P) and average grain size (D)
| x | a (Å) | c (Å) | V (Å3) | ρB (g/cm3) | ρth (g/cm3) | t | P (%) | D (μm) |
|---|---|---|---|---|---|---|---|---|
| 0.00 | 5.5457 | 13.7038 | 367 | 7.60 | 8.83 | 0.847 | 13.9 | 2.17 |
| 0.10 | 5.5790 | 13.6028 | 368 | 7.38 | 8.54 | 0.855 | 13.5 | 2.60 |
| 0.20 | 5.5859 | 13.5698 | 368 | 7.10 | 8.28 | 0.864 | 13.0 | 2.47 |
| 0.25 | 5.6001 | 13.7960 | 374 | 7.06 | 8.03 | 0.868 | 12.0 | 2.42 |
| x | Mr (emu/g) | Hc (kOe) | K (kOe emu/g) |
|---|---|---|---|
| 0.00 | 0.014 | 0.791 | 0.160 |
| 0.10 | 0.011 | 1.106 | 0.175 |
| 0.20 | 0.012 | 0.012 | 0.003 |
| 0.25 | 0.080 | 0.005 | 0.002 |
Table 2 Remnant magnetization (Mr), coercivity (Hc) and magnetic anisotropy (K) of xBST-(1 - x)BFGO ceramics at room temperature
| x | Mr (emu/g) | Hc (kOe) | K (kOe emu/g) |
|---|---|---|---|
| 0.00 | 0.014 | 0.791 | 0.160 |
| 0.10 | 0.011 | 1.106 | 0.175 |
| 0.20 | 0.012 | 0.012 | 0.003 |
| 0.25 | 0.080 | 0.005 | 0.002 |
Fig. 5 Variation of with frequency a, and Hc with BST content b and tanδ with frequency c of various xBST-(1 - x)BFGO ceramics sintered at 950 °C for 1 h
Fig. 6 Variation of ε' a and tanδb with frequency, and dependence of ε' c and tanδd on BST content of various xBST-(1 - x)BFGO ceramics sintered at 950 °C for 1 h
Fig. 8 Variation of Z′with frequency at room temperature for various xBST-(1 - x)BFGO ceramics a, and at different temperatures for 0.25BST-0.75BFGO ceramics b
| Temperature (°C) | Rg (kΩ) | Rgb (kΩ) | fr (kHz) | Cg (nF) | Cgb (nF) |
|---|---|---|---|---|---|
| 50 | 1060 | - | 1.09 | 0.14 | - |
| 100 | 1250 | - | 1.09 | 0.12 | - |
| 150 | 55 | 50 | 6.63 | 0.44 | 0.48 |
| 200 | 25 | 15 | 17.00 | 0.37 | 0.62 |
| 225 | 9.50 | 4.00 | 40.27 | 0.42 | 0.98 |
| 250 | 3.80 | 2.20 | 88.22 | 0.48 | 0.82 |
| 275 | 1.90 | 0.90 | 178.70 | 0.47 | 0.99 |
| 300 | 1.05 | 0.48 | 309.41 | 0.49 | 1.07 |
Table 3 Values for grain resistance (Rg), grain boundary resistance (Rgb), relaxation frequency (fr), grain capacitance (Cg) and grain boundary capacitance (Cgb) of 0.25BST-0.75BFGO
| Temperature (°C) | Rg (kΩ) | Rgb (kΩ) | fr (kHz) | Cg (nF) | Cgb (nF) |
|---|---|---|---|---|---|
| 50 | 1060 | - | 1.09 | 0.14 | - |
| 100 | 1250 | - | 1.09 | 0.12 | - |
| 150 | 55 | 50 | 6.63 | 0.44 | 0.48 |
| 200 | 25 | 15 | 17.00 | 0.37 | 0.62 |
| 225 | 9.50 | 4.00 | 40.27 | 0.42 | 0.98 |
| 250 | 3.80 | 2.20 | 88.22 | 0.48 | 0.82 |
| 275 | 1.90 | 0.90 | 178.70 | 0.47 | 0.99 |
| 300 | 1.05 | 0.48 | 309.41 | 0.49 | 1.07 |
Fig. 10 a Cole-Cole plots of Z′and Z′′at room temperature for different compositions of xBST-(1 - x)BFGO ceramics; b-i Cole-Cole plots for 0.25BST-0.75BFGO composition at different temperatures; j Arrhenius plots of grain and grain boundary conductivity for 0.25BST-0.75BFGO composition
Fig. 11 Variation of M′a and M'' b with frequency at various temperatures, Arrhenius plot of fmaxc, and M′versus M′′ curves at different temperatures d for 0.25BST-0.75BFGO composition sintered at 950 °C for 1 h
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