2017
DOI: 10.1016/j.jmmm.2016.09.103
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Structural and multiferroic properties of barium substituted bismuth ferrite nanocrystallites prepared by sol–gel method

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Cited by 29 publications
(9 citation statements)
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“…Figure 1(b) shows the FTIR spectra of BaFe 12 O 19 and Si‐BaFe 12 O 19 powder. It was found that both samples showed two strong absorption peaks at around 442 and 595 cm −1 assigned to FeO vibration and FeO stretching vibrations, respectively 22 . The Si‐BaFe 12 O 19 was confirmed by absorption peaks at around 1127 and 1049 cm −1 assigned to SiOH and SiOSi groups 23 and absorption peaks at around 3417 and 1630 cm −1 assigned to NH stretching and NH bending vibrations of the amine group, respectively 24 …”
Section: Resultsmentioning
confidence: 90%
See 1 more Smart Citation
“…Figure 1(b) shows the FTIR spectra of BaFe 12 O 19 and Si‐BaFe 12 O 19 powder. It was found that both samples showed two strong absorption peaks at around 442 and 595 cm −1 assigned to FeO vibration and FeO stretching vibrations, respectively 22 . The Si‐BaFe 12 O 19 was confirmed by absorption peaks at around 1127 and 1049 cm −1 assigned to SiOH and SiOSi groups 23 and absorption peaks at around 3417 and 1630 cm −1 assigned to NH stretching and NH bending vibrations of the amine group, respectively 24 …”
Section: Resultsmentioning
confidence: 90%
“…showed two strong absorption peaks at around 442 and 595 cm À1 assigned to Fe O vibration and Fe O stretching vibrations, respectively. 22 The Si-BaFe 12 O 19 was confirmed by absorption peaks at around 1127 and 1049 cm À1 assigned to SiO H and Si O Si groups 23 and absorption peaks at around 3417 and 1630 cm À1 assigned to N H stretching and N H bending vibrations of the amine group, respectively. 24 The surface morphology of BaFe 12 O 19 and Si-BaFe 12 O 19 is shown in Figures 2(a),(b), respectively.…”
Section: Characterization Of Magnetic Composite Filamentmentioning
confidence: 92%
“…These indicate that the intrinsic perovskite structures transform from the rhombohedral phase ( R 3 c ) into orthorhombic phase ( Pbnm ) by the doping of Ho/Ho and Ti, which show that the Bi (1.08 Å) and Fe (0.645 Å) sites are replaced by smaller ionic radius elements Ho (1.015 Å) and Ti (0.605 Å). , As x further increases up to 0.15 and 0.20, the diffraction peaks widen gradually, owing to the occurrence of structure transition from the rhombohedral ( R 3 c ) phase to a mixed state of cubic ( Pm 3̅ m ) and orthorhombic ( Pbnm ) phases. This is ascribed to the lattice distortion of BFO caused by the increase in chemical pressure of Ho and Ti. ,, The structural stability of the doped samples by Goldsmith tolerance factor ( t ) of the perovskite structure was reckoned by using this formula …”
Section: Resultsmentioning
confidence: 99%
“…[9] BFO displays a distorted rhombohedral structure and collinear anti-parallel spin arrangement of Fe ions, following zero macroscopic magnetization. [10] Spin canting of magnetic moments at the nanoparticle exterior is the origin of weak ferromagnetism or an (anti) ferromagnetic system. The weak ferromagnetism in BFO (x = 0) is due to the spin canting of magnetic moments.…”
Section: Magnetic Studiesmentioning
confidence: 99%
“…Ions of rare earth metals and alkaline earth metals (Mg, Ca, Ba, Sr, etc) have been used by many researchers to improve the multiferroic properties of BFO. [9,10] Due to the closeness in the ionic radius of strontium (1.18 Å) with bismuth (1.03 Å), Sr is the best choice of substitution at the bismuth site. From this substitution, a charge imbalance would be created that could be compensated in 3 ways: (i) creation of oxygen vacancies, (ii) charge discrepancy of Fe 3+ and Fe 5+ , and (iii) partial transformation of Fe 3+ to Fe 4+ .…”
Section: Introductionmentioning
confidence: 99%