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by Martin Greven and John Arthur | ||
The strong
electron correlations in transition metal oxides give rise to such phenomena
as high-temperature superconductivity in layered cuprates and to stripe-like
order in layered cuprates and nickelates. In the case of the manganites,
an additional strong electron-lattice interaction leads to a very rich
phase diagram in which structural, magnetic, and transport properties are
intimately related. Colossal magnetoresistance (CMR) has been observed
in the perovskite and double-layer manganites, but not in the single-layer
system La1-xSr1+xMnO4 (Mn214).
Nevertheless, there are signs that the physics of Mn214 is similar to that
of the perovskites. Information about the low-temperature structural phases
of Mn214 can be expected to provide valuable insight into the role of dimensionality
on the properties of the manganites, and also to contribute to a deeper
understanding of single-layer transition metal oxides in general.
Simon Larochelle and co-workers have grown single crystals at Stanford's new Laboratory for Advanced Materials and carried out x-ray scattering studies at SSRL Beamline 7-2 to establish the low-temperature structural phase diagram of Mn214 [1]. For x = 1/2, this study provides a more complete picture than previous neutron [2] and x-ray [3] scattering experiments. An investigation of the effects of varying the eg electron concentration (ne = 1 - x) in the MnO2 layers revealed three distinct regions: disordered (x < 0.4), mixed-phase (0.4 < x < 0.5), and charge-ordered (x >0.5). Above x = 0.5, the ordering of eg electrons is found to result in a structural distortion whose modulation period only depends on ne. Even though Mn214 does not exhibit CMR, this trend resembles findings for La1-xCaxMnO3, which is a CMR material. This behavior furthermore is reminiscent of the charge- and spin-density wave order tendencies in the hole-doped layered cuprates and nickelates. The results of this study thus provide valuable quantitative information for tests of theories for CMR materials and layered transition metal oxides. |
![]() (a) Superlattice wave vector (±e, 0, 0)o as a function of x for La1-xSr1+xMnO4. The dashed line for x > 0.5 is e = 2(1 - x) = 2ne. (b) Linear-scale contour map (10% contours) of the scattering intensity around (10, 6, 0)o for x = 0.525. ![]() H scans through the (8, 4, 0)o and (9, 4, 0)o reflections for x = 0.40, 0.45, and 0.50 (T = 100 K). The (8, 4, 0)o peak intensities are normalized to 106. Below x=0.50, the (9, 4, 0)o superlattice peak intensity decreases considerably with decreasing x. For x = 0.40, the peak is noticeably broadened and its intensity is ~104 weaker than for x = 0.50 reflecting mixed-phase behavior |
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References
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Last Updated: | 28 SEP 2001 |
Content Owners: | M. Greven and J. Arthur | |
Page Editor: | Lisa Dunn |