Publication | Closed Access
Structure, Magnetism, and Properties of Ruddlesden−Popper Calcium Manganates Prepared from Citrate Gels
118
Citations
18
References
1998
Year
Magnetic PropertiesEngineeringMagnetic ResonanceEffective Magnetic MomentChemistryInorganic MaterialMagnetic MaterialsMagnetismCalcium AluminateCitrate GelsMaterials ScienceInorganic ChemistryMagnetic MaterialCrystallographyFerromagnetismMno6 DeformationNatural SciencesMagnetic PropertySpontaneous Magnetic Ordering
Ruddlesden−Popper (RP) phases with the formula (CaO)(CaMnO3)n, where n = 1, 2, 3, and ∞, have been prepared using the Pechini citrate gel process at temperatures as low as 900 °C under flowing oxygen. The compounds were characterized by X-ray powder diffraction, Rietveld profile analysis, thermal gravimetric analysis, iodometric titrations, Mn K-edge X-ray absorption spectroscopy, temperature-dependent magnetic susceptibility, and resistivity. Rietveld analysis shows that there is an elongation in the apical Mn−O distances of the MnO6 octahedra, which increases with decreasing dimensionality. Mn K-edge X-ray absorption spectroscopy and iodometric titrations show no detectable amount of Mn3+ (a Jahn−Teller distorted d4 ion) in the samples indicating that the MnO6 deformation may be associated with a splitting in the half-filled t2g levels of Mn4+. Magnetic susceptibility measurements show spontaneous magnetic ordering to antiferromagnetic states at ∼125 K for CaMnO3 and Ca4Mn3O10 and at ∼110 K for Ca2MnO4 and Ca3Mn2O7. The effective magnetic moment is greatly suppressed in all of the RP manganates, even in the three-dimensional CaMnO3, n = ∞ phase, and decreases dramatically with decreasing dimensionality. Large deviations from Curie−Weiss behavior are observed above the ordering temperature, which increase with decreasing n. These observations are discussed in terms of two-dimensional magnetic fluctuations and alternative mechanisms. The compounds are all poor electronic conductors with room-temperature resistivities in the range of 102−104 Ω cm.
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