Abstract:Ca x Sr 1-x Bi 2 Nb 2 O 9 , as one of Aurivillius ceramics, was prepared by a conventional solid-state reaction method. The X-ray diffraction study showed that the ceramic possess a pure structure and no secondary phase can be detected. The scanning electron microscopy indicates that the grains of all the samples are all welldefined, but no obvious impact on the size of the ceramics. The dielectric, ferroelectric and piezoelectric properties of the Ca 0.1 Sr 0.9 Bi 2 Nb 2 O 9 were investigated and found that t… Show more
“…Meanwhile, it is obvious that the highest diffraction peak in KCSNBT-x ceramics corresponds to the (1011) orientation, which is consistent with the fact that it is the strongest diffraction peak in BLSFs. 16 In addition to the main Aurivillius phase, secondary phase Bi 2 Ti 2 O 7 (PDF#no. 32-0118, labeled by *) in the KCSNBT-x samples can also be detected regardless of the existence of (KCe), as shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…where A is a pre-exponential factor constant, E a is the activation energy of the mobile charge carriers, k B is the Boltzmann constant and T is the absolute temperature. 16 The activation energy is shown in the inset of Fig. 4 and Table 2.…”
Bismuth layer-structured ferroelectrics with a formula of Sr1−x(K,Ce)x/2(Na0.5Bi0.5)Bi4Ti5O18, were prepared by a conventional solid-state reaction method.
“…Meanwhile, it is obvious that the highest diffraction peak in KCSNBT-x ceramics corresponds to the (1011) orientation, which is consistent with the fact that it is the strongest diffraction peak in BLSFs. 16 In addition to the main Aurivillius phase, secondary phase Bi 2 Ti 2 O 7 (PDF#no. 32-0118, labeled by *) in the KCSNBT-x samples can also be detected regardless of the existence of (KCe), as shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…where A is a pre-exponential factor constant, E a is the activation energy of the mobile charge carriers, k B is the Boltzmann constant and T is the absolute temperature. 16 The activation energy is shown in the inset of Fig. 4 and Table 2.…”
Bismuth layer-structured ferroelectrics with a formula of Sr1−x(K,Ce)x/2(Na0.5Bi0.5)Bi4Ti5O18, were prepared by a conventional solid-state reaction method.
“…1,2 Bismuth layer structure Ferroelectric (BLSF) ceramics have been investigated because of their high Curie temperature (T c ), lower dielectric loss, excellent fatigue properties and short aging rates. [3][4][5][6][7] Among BLSFs, SBN has received special attention because it retains its structure even after doping compared to other Arivullius oxides of the bismuth layer. 8,9 SBN has a typical bismuth layer structure in which blocks of perovskite (SrNb 2 O 7 ) 2− , made up of double octahedra of NbO 6 are interwoven with layers of (Bi 2 O 2 ) 2+ .…”
Lead free dielectric materials of Strontium Bismuth Niobate SrBi2Nb2O9 (SBN) and rare earth double doped SrBi1.8Pr0.1Gd0.1Nb2O9 (SBPGN), SrBi1.8Pr0.1Y0.1Nb2O9 (SBPYN), SrBi1.8Eu0.1Gd0.1Nb2O9 (SBEGN) and SrBi1.8Eu0.1Y0.1Nb2O9 (SBEYN) were prepared by two-stage solid-state reaction route. The XRD studies have confirmed the formation of single-phase orthorhombic crystal structure. The microstructural analysis showed the formation of plausible needle shaped grains in the prepared ceramics. The FTIR study was used to investigate the effect of preparation and doping processes on the band intensities of the spectra. Mechanical studies showed that SBEGN and SBEYN ceramics exhibited mild wear (<10−6 mm3 Nm−1) compared to others. The low friction coefficient values of SBPYN (0.044), SBEGN (0.058) and SBEYN (0.002) to that of SBN necessitate lattice strain in these materials. The VSM studies on the rare earth double doped SBN ceramic materials confirmed the induction and existence of magnetic order in SBPGN and SBEGN.
“…where A is a pre-exponential factor constant, E a is the activation energy of the mobile charge carriers, k B is the Boltzmann constant and T is the absolute temperature. 26 The activation energy is shown in the inset of Fig. 5 and Table 1.…”
Lead-free piezoelectric ceramics with the formula of Sr1−x(Li,Ce)x/2(Na0.5Bi0.5)Bi4Ti5O18 (LCSNBT-x, x = 0.0, 0.1, 0.2, 0.3, 0.4), were prepared by a conventional solid-state reaction method.
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