2000
DOI: 10.1016/s0921-4526(99)01761-5
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Neutron diffraction and mössbauer effect study of quenched 112CdFe2O4

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“…The cation distribution in such materials is typically represented by the inversion parameter, λ, with (A 1−λ B λ ) tet (A λ B 2−λ ) oct O 4 . In a normal spinel such as microcrystalline CdFe 2 O 4 (see inset of Figure 5b), which shows virtually no inversion (λ ≈ 0.05), 47 the single A cation occupies the tetrahedral 8a Wyckoff site while the two B cations are located on two equivalent octahedral 16d sites. In contrast, in an inverse spinel such as microcrystalline CoFe 2 O 4 , one of the B cations is located on the tetrahedral site while both the single A cation and the other B cation occupy the two octahedral coordination sites randomly.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
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“…The cation distribution in such materials is typically represented by the inversion parameter, λ, with (A 1−λ B λ ) tet (A λ B 2−λ ) oct O 4 . In a normal spinel such as microcrystalline CdFe 2 O 4 (see inset of Figure 5b), which shows virtually no inversion (λ ≈ 0.05), 47 the single A cation occupies the tetrahedral 8a Wyckoff site while the two B cations are located on two equivalent octahedral 16d sites. In contrast, in an inverse spinel such as microcrystalline CoFe 2 O 4 , one of the B cations is located on the tetrahedral site while both the single A cation and the other B cation occupy the two octahedral coordination sites randomly.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…Fig. 5b), which shows virtually no inversion (λ ≈ 0.05), [47] the single A cation occupies the tetrahedral 8a Wyckoff site while the two B cations are located on two equivalent octahedral 16d sites.…”
Section: Fig S3 In Esi)mentioning
confidence: 99%