Mixed-valence manganites with the ABO3 perovskite structure display a variety of magnetic and structural transitions, dramatic changes of electrical conductivity and magnetoresistance effects. The physical properties vary with the relative concentration of Mn3+ and Mn4+ in the octahedral corner-sharing network, and the proportion of these two cations is usually changed by doping the trivalent large A cation (for example, La3+) with divalent cations. As the dopant and the original cation have, in general, different sizes, and as they are distributed randomly in the structure, such systems are characterized by local distortions that make it difficult to obtain direct information about their crystallographic and physical properties. On the other hand, the double oxides of formula AA'3Mn4O12 contain a perovskite-like network of oxygen octahedra centred on the Mn cations, coupled with an ordered arrangement of the A and A' cations, whose valences control the proportion of Mn3+ and Mn4+ in the structure. The compound investigated in this work, (NaMn3+(3))(Mn3+(2)Mn4+(2))O12, contains an equal number of Mn3+ and Mn4+ in the octahedral sites. We show that the absence of disorder enables the unambiguous determination of symmetry, the direct observation of full, or nearly full, charge ordering of Mn3+ and Mn4+ in distinct crystallographic sites, and a nearly perfect orbital ordering of the Mn3+ octahedra.
The BiMnO3 perovskite is a very interesting multiferroic material that, once synthesized at high pressure
and high temperature, survives as a metastable phase at ambient conditions. We investigated ceramic
samples prepared in different conditions (temperature, pressure, and composition), and the existence of
polymorphism at room temperature was clearly evidenced by electron diffraction and high-resolution
electron microscopy in all the samples. A new polymorph, characterized by a different distortion of the
perovskite basic cell, was found to coexist as a minor phase with the well-known C2 monoclinic form.
The new polymorph, which can be described by a triclinic (pseudorhombohedral) superstructure with a
= 13.62 Å, b = 13.66 Å, c = 13.66 Å, α = 110.0°, β = 108.8°, and γ = 108.8°, is mostly segregated
at the grain surface. Magnetic characterizations revealed for this second form a critical temperature of
107 K, a few degrees above the ferromagnetic transition of the monoclinic C2 form measured at 99 K.
The new phase disappears by reheating the samples at ambient pressure, suggesting the idea of a higher
energy polymorph, which kinetically converts in the usual phase once a sufficient temperature has been
achieved.
The multiferroic perovskite BiMnO3, synthesized under high-pressure conditions, decomposes if heated
at room-pressure in the temperature range of 500−650 °C. Comparative studies by high-temperature
X-ray diffraction, electron diffraction, thermal analysis, and magnetic investigation revealed the existence
of a complex pathway to decomposition, depending on the heating rate, pressure, and atmosphere that
involves different metastable phases. In particular the as-prepared monoclinic phase (I) transforms to a
second monoclinic form (II) at 210 °C and then to an orthorhombic phase (III) at 490 °C. These phase
transitions, fast and reversible, occur on heating with a drop in volume and are moved at higher
temperatures when pressure is decreased. The transition from II to III, typically observed in inert
atmosphere, can be detected also in air when the heating rate is kept sufficiently high. When III is heated
in an oxygen-containing atmosphere a slow irreversible transition to variants IV and then V takes place
with kinetics depending on temperature, heating rate, and oxygen partial pressure. Both IV and V are
oxidized ferromagnetic phases containing Mn4+ characterized by a modulated structure based on
fundamental triclinic perovskite cells. Their magnetic behavior shows a strong analogy with thin films
of BiMnO3, suggesting for the latter an oxidized nature and for the former a possible multiferroic behavior.
We have prepared perpendicular hard/soft bilayers made of a 10nm L10-FePt layer, which has been epitaxially grown on MgO(100) and a Fe layer with thicknesses of 2 and 3.5nm. The control of the interface morphology allows to modify the magnetic regime at fixed Fe thickness (from rigid magnet to exchange-spring magnet), due to the nanoscale structure effect on the hard/soft coupling and to tailor the hysteresis loop characteristics. Despite the small thickness of the soft layer, the coercivity is strongly reduced compared to the hard layer value, indicating that high anisotropy perpendicular systems with moderate coercivity can be easily obtained.
We report on a systematic study of the structural, magnetic and transport properties of highpurity 1T-VS 2 powder samples prepared under high pressure. The results differ notably from those previously obtained by de-intercalating Li from LiVS 2 . First, no Charge Density Wave (CDW) is found by transmission electron microscopy down to 94 K. Though, ab initio phonon calculations unveil a latent CDW instability driven by an acoustic phonon softening at the wave vector q CDW ≈ (0.21,0.21,0) previously reported in de-intercalated samples. A further indication of latent lattice instability is given by an anomalous expansion of the V-S bond distance at low temperature.Second, infrared optical absorption and electrical resistivity measurements give evidence of non metallic properties, consistent with the observation of no CDW phase. On the other hand, magnetic susceptibility and NMR data suggest the coexistence of localized moments with metallic carriers, in agreement with ab initio band structure calculations. This discrepancy is reconciled by a picture of electron localization induced by disorder or electronic correlations leading to a phase separation of metallic and non-metallic domains in the nm scale. We conclude that 1T-VS 2 is at the verge of a CDW transition and suggest that residual electronic doping in Li de-intercalated samples stabilizes a uniform CDW phase with metallic properties.
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