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Magnetic materials are composed of the simple building blocks of magnetic moments on a crystal lattice that interact via magnetic exchange. Yet from this simplicity emerges a remarkable diversity of magnetic states. Some reveal the deep quantum mechanical origins of magnetism, for example, quantum spin liquid (QSL) states in which magnetic moments remain disordered at low temperatures despite being strongly correlated through quantum entanglement. A promising theoretical model of a QSL is the Kitaev model, composed of unusual bond-dependent exchange interactions, but experimentally, this model is challenging to realise. Here we show that the material requirements for the Kitaev QSL survive an extended pseudo-edge-sharing superexchange pathway of Ru octahedra within the honeycomb layers of the inorganic framework solid, RuPSiO. We confirm the requisite state of Ru in RuPSiO and resolve the hierarchy of exchange interactions that provide experimental access to an unexplored region of the Kitaev model.
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http://dx.doi.org/10.1038/s41467-024-53900-3 | DOI Listing |
J Phys Chem A
September 2025
Department of Chemistry, Tsinghua University, Beijing 100084, China.
A series of Cu-based single-atom catalysts (SACs) with asymmetric coordination were designed to accelerate lithium-sulfur (Li-S) chemistry. The electronegativity contrast from the dopant induces a localized electronic asymmetry that amplifies Jahn-Teller distortion at the Cu center. This distortion profoundly modulates the Cu 3d electronic structure and its interaction with Li-S intermediates.
View Article and Find Full Text PDFPhys Chem Chem Phys
September 2025
School of Physics, Nanjing University of Science and Technology, Nanjing 210094, China.
Multifunctional materials that simultaneously possess intrinsic magnetic and superhard properties, particularly those composed of light elements, have a wide range of applications in advanced sensors, shielding, durable devices, and other fields. However, research on the development and understanding of such materials remains limited. In this study, a series of 3D C covalent networks derived from the C fullerene precursor were theoretically designed.
View Article and Find Full Text PDFPhys Chem Chem Phys
September 2025
Masaryk University, Faculty of Science, Department of Chemistry, Kotlářská 2, Brno, 611 37, Czech Republic.
Structural and magnetic properties of ultra-small tetrahedron-shaped iron oxide nanoparticles were investigated using density functional theory. Tetrahedral and truncated tetrahedral models were considered in both non-functionalized form and with surfaces passivated by pseudo-hydrogen atoms. The focus on these two morphologies reflects their experimental relevance at this size scale and the feasibility of performing fully relaxed, atomistically resolved first-principles simulations.
View Article and Find Full Text PDFSci Technol Adv Mater
August 2025
Research Center for Magnetic and Spintronic Materials, National Institute for Materials Science (NIMS), Tsukuba, Japan.
Emergent ferromagnetism on the surface of two-dimensional (2D) MXene is investigated by X-ray magnetic circular dichroism (XMCD) and angle-dependent hard X-ray photoemission spectroscopy (HAXPES). Focusing on CrN as one of the 2D-MXenes, high quality bilayers of CrN/Co and CrN/Pt are prepared by a magnetron sputtering technique. XMCD reveals the induced magnetic moment of Cr in the CrN/Co interface, while it is not observed in the CrN/Pt interface at room temperature.
View Article and Find Full Text PDFInorg Chem
September 2025
Department of Chemistry and Biochemistry, University of South Carolina, Columbia, South Carolina 29208, United States.
A series of six quinary rare-earth sulfides CeEuNaSiS, CeEuKSiS, CeEuRbSiS, CeEuCsSiS, CeEuAgSiS, and CeEuCuSiS were obtained in an alkali iodide flux using the boron-chalcogen mixture (BCM) method. Single crystal X-ray diffraction was used to determine the structures of the high quality single crystals that were grown; their elemental compositions were confirmed by energy-dispersive spectroscopy (EDS). The compounds crystallize in the hexagonal crystal system in the noncentrosymmetric space group 6.
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