98%
921
2 minutes
20
Polycrystalline samples of Ln18Li8Rh5O39 (Ln = La, Pr) have been synthesized by the ceramic method and characterized by X-ray and neutron diffraction. The compounds crystallize in the cubic space group Pmn, with a0 approximately 12.1 Angstroms. The unit cell contains four intersecting 111 chains, each comprised of an alternating sequence of face-sharing RhO6 octahedra and LiO6 trigonal prisms. The octahedra located at the points of intersection contain Rh4+, whereas the remainder contain Rh3+; the compounds thus contain a charge-ordered arrangement of the two cations. The polyhedral chains are enclosed in tunnels formed by the Ln-O sublattice. The magnetic properties of the two new compounds are discussed briefly: both are paramagnetic over the temperature range 5 < TK < 300.
Download full-text PDF |
Source |
---|---|
http://dx.doi.org/10.1021/ic050949s | DOI Listing |
Phys Rev Lett
January 2025
Aalto University, Department of Applied Physics, FI-00076 Aalto, Finland.
The doped Hubbard model is one of the paradigmatic platforms to engineer exotic quantum many-body states, including charge-ordered states, strange metals, and unconventional superconductors. While undoped and doped correlated phases have been experimentally realized in a variety of twisted van der Waals materials, experiments in monolayer materials, and in particular 1T transition metal dichalcogenides, have solely reached the conventional insulating undoped regime. Correlated phases in monolayer two-dimensional materials have much higher associated energy scales than their twisted counterparts, making doped correlated monolayers an attractive platform for high temperature correlated quantum matter.
View Article and Find Full Text PDFInorg Chem
January 2024
Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan.
FeGeTe is a two-dimensional van der Waals material that exhibits ferromagnetic order with a high Curie temperature () of around room temperature. In addition to , two magnetic transitions occur with decreasing temperature, and a charge-ordered state is observed at low temperatures. We employed Ge Kα X-ray fluorescence holography (XFH) for FeGeTe to directly investigate the local structure in the charge-ordered state, i.
View Article and Find Full Text PDFInorg Chem
August 2023
School of Materials Science and Engineering, Jiangsu University of Science and Technology, 212100 Zhenjiang, Jiangsu, China.
Nat Commun
June 2021
School of Applied and Engineering Physics, Cornell University, Ithaca, NY, USA.
The self-organization of strongly interacting electrons into superlattice structures underlies the properties of many quantum materials. How these electrons arrange within the superlattice dictates what symmetries are broken and what ground states are stabilized. Here we show that cryogenic scanning transmission electron microscopy (cryo-STEM) enables direct mapping of local symmetries and order at the intra-unit-cell level in the model charge-ordered system NdSrMnO.
View Article and Find Full Text PDFPhys Rev Lett
August 2018
School of Physics and Astronomy and Centre for Science at Extreme Conditions, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
RbFe^{2+}Fe^{3+}F_{6} is an example of a charge ordered antiferromagnet where iron sites, with differing valences, are structurally separated into two interpenetrating sublattices. The low temperature magnetically ordered Fe^{2+} (S=2) and Fe^{3+} (S=5/2) moments form a noncollinear orthogonal structure with the Fe^{3+} site displaying a reduced static ordered moment. Neutron spectroscopy on single crystals finds two distinct spin wave branches with a dominant coupling along the Fe^{3+} chain axis (b axis).
View Article and Find Full Text PDF