1992
DOI: 10.1016/0304-8853(92)90255-m
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Calculated electronic band structure and magnetic moments of ferrites

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Cited by 149 publications
(71 citation statements)
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“…[33][34][35] The tetrahedral and octahedral sites are antiferromagnetically coupled; resulting in a magnetic moment varying between 3.65 -4.43 μ B , depending on the theoretical model. 11,12,14,15,36 Hence, magnetite is a ferrimagnet, with a large critical temperature of T c = 858 K.…”
Section: Introductionmentioning
confidence: 99%
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“…[33][34][35] The tetrahedral and octahedral sites are antiferromagnetically coupled; resulting in a magnetic moment varying between 3.65 -4.43 μ B , depending on the theoretical model. 11,12,14,15,36 Hence, magnetite is a ferrimagnet, with a large critical temperature of T c = 858 K.…”
Section: Introductionmentioning
confidence: 99%
“…Cobalt ferrite, like magnetite, is ferrimagnetic with a magnetic moment predicted by different theoretical models to be between 2.73 -3 µ B /f.u. for a perfect inverse spinel crystal structure; 11,12,15 the magnetic moment will increase with increased mixing of the Co 2+ cations between the octahedral and tetrahedral sites. Cobalt ferrite has a large magnetic anisotropy due to a spin-orbit stabilized doublet (with unquenched orbital momentum l z = ±1) ground state caused by a trigonal crystal field on the Co 2+ octahedral cations, 27, 39-45 with a cubic magnetocrystalline anisotropy constant, K 1 , which is positive and larger by over an order of magnitude than the other 3d-transition-metal spinel ferrites.…”
Section: Introductionmentioning
confidence: 99%
“…(1)), hence any error in point-charge estimates used in our EFG model amplifies the errors of η entered into Eqs. (3). No temperature evolution was assumed in the charge-ordered state below T V , and the set was solved for the temperature 20 K where precise crystal-structure data exist [11].…”
Section: Solving the Set Of Eqs (3) Into Occupanciesmentioning
confidence: 99%
“…Positive populations could be obtained for both orientations allowed by β = 90°, Above T = 433 K N , the equality for the internal field disappears from the set of Eqs. (3). Considering the smooth evolution above T p towards the small positive eQV zz of the valence-mixed phase, the orbital populations can be extrapolated into the paramagnetic phase at T N .…”
Section: Implications For Efg Above T Pmentioning
confidence: 99%
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