2022
DOI: 10.1103/physrevb.106.054416
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Temperature dependence of the local electromagnetic field at the Fe site in multiferroic bismuth ferrite

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Cited by 7 publications
(4 citation statements)
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“…Although BFO exhibits the magnetoelectric effect at room temperature, as confirmed in measurements with hyperfine interaction techniques [5,6], the magnetoelectric coupling in BFO is too weak for practical applications, due to a modification of the antiferromagnetic G-type spin configuration by a long-range spiral spin superstructure. This spiral spin superstructure cancels the macroscopic magnetization and, thus, prevents a linear magnetoelectric effect.…”
Section: Introductionmentioning
confidence: 96%
“…Although BFO exhibits the magnetoelectric effect at room temperature, as confirmed in measurements with hyperfine interaction techniques [5,6], the magnetoelectric coupling in BFO is too weak for practical applications, due to a modification of the antiferromagnetic G-type spin configuration by a long-range spiral spin superstructure. This spiral spin superstructure cancels the macroscopic magnetization and, thus, prevents a linear magnetoelectric effect.…”
Section: Introductionmentioning
confidence: 96%
“…Nonetheless, the primary drawback associated with the current photocatalysts lies in their wide band gap, deep trap states, rapid recombination of charge carriers, surface reconstruction, and nonreproducibility. , Furthermore, the synthesis conditions for these oxide-based photocatalysts are exceptionally harsh and time-consuming, necessitating high temperatures and pressures. Hence, the synthesis process is energy-intensive and cost-ineffective. Consequently, due to these aforementioned limitations, the practical commercialization of these existing photocatalysts is unfeasible owing to their inefficient catalytic performances.…”
Section: Introductionmentioning
confidence: 99%
“…Meanwhile, the relationship B hf = αM is usually linear for 57 Fe, 55 Mn, and 53 Cr nuclei, and the dependencies of the EFG tensor parameters V ii = f(P s ) and η = f ′ (P s ) (where η = (V XX − V YY )/V ZZ is the asymmetry parameter) demonstrate nontrivial behavior. In some works, quadratic dependences V ii = a + bP s 2 and η ∝ P s 2 are used for approximation [31][32][33]. However, such an approach is rather formal and does not allow for associating the hyperfine parameters of different resonant nuclei with the structural data and physical characteristics of the compounds under study.…”
Section: Introductionmentioning
confidence: 99%