“…According to Fisher et al ., 11 excess TiO 2 and inhomogeneities of additives promoted abnormal grain growth in BaTiO 3 . However, no new phases and abnormal grain growth occurred in 3.5 and 5.0 mol% Mg ‐doped samples.…”
The photoluminescence of Mg‐doped BaTiO3:Pr3+ (Pr3+: 0.1 mol%) ceramics was investigated by changing the doping concentration of Mg and the sintering temperature. The results indicated that the intensity of red emission due to the 1D2→3H4 transition of Pr3+ exhibited significant dependence on both the Mg doping content and the sintering temperature; the strongest red emission intensity was observed for 2.0 mol% Mg‐doped ceramics sintered at 1050°C. An interpretation of the results obtained was made in terms of the changes in the crystal structure and microstructure of the ceramics.
“…According to Fisher et al ., 11 excess TiO 2 and inhomogeneities of additives promoted abnormal grain growth in BaTiO 3 . However, no new phases and abnormal grain growth occurred in 3.5 and 5.0 mol% Mg‐doped samples.…”
The photoluminescence of Mg‐doped BaTiO3:Pr3+ (Pr3+: 0.1 mol%) ceramics was investigated by changing the doping concentration of Mg and the sintering temperature. The results indicated that the intensity of red emission due to the 1D2→3H4 transition of Pr3+ exhibited significant dependence on both the Mg doping content and the sintering temperature; the strongest red emission intensity was observed for 2.0 mol% Mg‐doped ceramics sintered at 1050°C. An interpretation of the results obtained was made in terms of the changes in the crystal structure and microstructure of the ceramics.
“…4(a)), the grain has the angular shape with the flat surface, which is typically observed in the microstructure with abnormal grain growth (AGG). It is generally agreed that AGG is caused by the existence of a liquid phase [21][22][23]. Zhen et al [23] found that extensive AGG occurred on the (Li 0.04 K 0.44 Na 0.52 )NbO 3 and (Li 0.04 K 0.44 Na 0.52 )(Nb 0.85 Ta 0.15 )O 3 ceramics and concluded that the volatilization of alkali components was responsible for the occurrence of AGG.…”
0.94(K 05 Na 0.5 )NbO 3 −0.03LiNbO 3 −0.03LiSbO 3 (KNLNS) lead-free piezoelectric ceramics were prepared by conventional mixed oxide route with normal sintering method. The samples were sintered at different temperatures with KNLNS powder atmosphere to prevent volatilization of alkali metal oxides at high temperature. The effects of sintering temperature on the density, structure and electric properties of KNLNS ceramics were studied. X-ray diffraction (XRD) results showed that the crystal structure of the crushed KNLNS ceramic powders were pure perovskite phase with tetragonal phase structure when sintered at T≤1080°C. However a K 3 Li 2 Nb 5 O 15 phase with tetragonal tungsten bronze structure began to appear when the sintering temperature was higher than 1080°C. The optimum sintering temperature was 1080°C which was determined by measuring the density of the samples. Scanning electron microscope (SEM) observation indicated that the sintering temperature had a great effect on the microstructure of the samples. The KNLNS ceramics under the optimum sintering temperature showed excellent electric properties: ρ=4.29 g/cm 3 , ε r =826, tanδ=0.049, d 33 =190 pC/N, k p =0.30, and T c =385°C. The results show that the KNLNS ceramics are promising candidate for lead-free piezoelectric ceramics.
“…In this work, we shall study the effect of Al 2 O 3 additions on abnormal grain growth in BaTiO 3 sintered above the BaTiO 3 –Ba 6 Ti 17 O 40 eutectic temperature. The affect of Al 2 O 3 on abnormal grain growth in BaTiO 3 samples sintered below the eutectic temperature has been described in a previous paper 22 …”
The effect of additions of ≤1 mol% Al2O3 on abnormal grain growth in BaTiO3 sintered for periods of ≤60 min at 1350°C has been studied. Addition of ≤0.2 mol% Al2O3 caused an increase in the nucleation and growth rates of abnormal grains, with further additions causing a decrease. This behavior is explained by interface‐controlled growth. Dopant adsorption reduces both the edge free energy and the step velocity of a grain, causing the nucleation and growth rates of abnormal grains to increase, pass through a maximum, and then decrease with increasing dopant concentration.
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