2017
DOI: 10.1007/s11664-016-5248-0
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Origin of Room Temperature Ferromagnetism in Cr-Doped Lead-Free Ferroelectric Bi0.5Na0.5TiO3 Materials

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Cited by 61 publications
(36 citation statements)
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“…Figure 3(a) presents the optical absorbance spectra of undoped Bi 0.5 Na 0.5 TiO 3 and CaFeO 3-δ -modified Bi 0.5 Na 0.5 TiO 3 materials at various concentrations at room temperature. The pure Bi 0.5 Na 0.5 TiO 3 samples exhibited a single absorbance edge, which is consistent with the recently reported optical properties of Bi 0.5 Na 0.5 TiO 3 materials 29,30,50,51 . The addition of CaFeO 3-δ to Bi 0.5 Na 0.5 TiO 3 caused the absorbance edge to shift to high wavelengths, indicating that the electronic band structures had been modified.…”
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confidence: 91%
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“…Figure 3(a) presents the optical absorbance spectra of undoped Bi 0.5 Na 0.5 TiO 3 and CaFeO 3-δ -modified Bi 0.5 Na 0.5 TiO 3 materials at various concentrations at room temperature. The pure Bi 0.5 Na 0.5 TiO 3 samples exhibited a single absorbance edge, which is consistent with the recently reported optical properties of Bi 0.5 Na 0.5 TiO 3 materials 29,30,50,51 . The addition of CaFeO 3-δ to Bi 0.5 Na 0.5 TiO 3 caused the absorbance edge to shift to high wavelengths, indicating that the electronic band structures had been modified.…”
supporting
confidence: 91%
“…Ferromagnetism in Fe-doped Bi 0.5 Na 0.5 TiO 3 materials is an intrinsic phenomenon, whereas ferromagnetism in Co-doped Bi 0.5 Na 0.5 TiO 3 materials is due to the presence of magnetic Co clusters 27,28 . Thanh et al reported that Mn-and Cr-doped Bi 0.5 Na 0.5 TiO 3 materials possibly influence room-temperature ferromagnetism 29,30 . On the other hand, the room-temperature ferromagnetic properties in Mn-doped Bi 0.5 Na 0.5 TiO 3 materials result from an interaction of the Mn cation through O vacancies, whereas those in Cr-doped Bi 0.5 Na 0.5 TiO 3 materials were mostly related to self-defects and enhancement via O vacancies 29,30 .…”
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