Direct observation of electron density reconstruction at the metal-insulator transition in NaOsO3
arXiv:1803.08271 · doi:10.1103/PhysRevB.98.115116
Abstract
5d transition metal oxides offer new opportunities to test our understanding of the interplay of correlation effects and spin-orbit interactions in materials in the absence of a single dominant interaction. The subtle balance between solid-state interactions can result in new mechanisms that minimize the interaction energy, and in material properties of potential use for applications. We focus here on the 5d transition metal oxide NaOsO3, a strong candidate for the realization of a magnetically driven transition from a metallic to an insulating state exploiting the so-called Slater mechanism. Experimental results are derived from non-resonant and resonant x-ray single crystal diffraction at the Os L-edges. A change in the crystallographic symmetry does not accompany the metal-insulator transition in the Slater mechanism and, indeed, we find no evidence of such a change in NaOsO3. An equally important experimental observation is the emergence of the (300) Bragg peak in the resonant condition with the onset of magnetic order. The intensity of this space-group forbidden Bragg peak continuously increases with decreasing temperature in line with the square of intensity observed for an allowed magnetic Bragg peak. Our main experimental results, the absence of crystal symmetry breaking and the emergence of a space-group forbidden Bragg peak with developing magnetic order, support the use of the Slater mechanism to interpret the metal-insulator transition in NaOsO3. We successfully describe our experimental results with simulations of the electronic structure and, also, with an atomic model based on the established symmetry of the crystal and magnetic structure.
arXiv comment6 figures
References in corpus (24)
- Mott Insulators in the Strong Spin-Orbit Coupling Limit: From Heisenberg to a Quantum Compass and Kitaev Models
- Novel Jeff = 1/2 Mott State Induced by Relativistic Spin-Orbit Coupling in Sr2IrO4
- Quantum spin Hall effect in a transition metal oxide Na2IrO3
- Direct observation of orbital ordering in LaSrMnO using soft x-ray diffraction
- Magnetically driven metal-insulator transition in NaOsO3
- Continuous metal-insulator transition of the antiferromagnetic perovskite NaOsO3
- Orbital ordering transition in CaRuO observed with resonant x-ray diffraction
- Electromagnetic properties and electronic structure of iron-based layered superconductor LaOFeP
- Resonant X-ray scattering and the electronic ground state in iridate perovskites
- Resonant Soft X-ray Scattering Investigation of Orbital and Magnetic Ordering in
- Confinement-Deconfinement Transition as an Indication of Spin-Liquid-Type Behavior in NaIrO
- Effect of Spin-Orbit Interaction on (4d)^3- and (5d)^3 -Based Transition-Metal Oxides
- Electronic structure and magnetic properties of NaOsO
- Lifshitz transition driven by spin fluctuations and spin-orbit renormalization in NaOsO
- Experimental evidence of anapolar moments in the antiferromagnetic insulating phase of V2O3 obtained from x-ray resonant Bragg diffraction
- Structural and Correlation Effects in the Itinerant Insulating Antiferromagnetic Perovskite NaOsO3
- Infrared evidence of a Slater metal-insulator transition in NaOsO3
- Direct observation of oxygen superstructures in manganites
- Strongly Gapped Spin-Wave Excitation in the Insulating Phase of NaOsO3
- Dzyaloshinsky-Moriya driven helical-butterfly structure in Ba3NbFe3Si2O14
- Evolution of the magnetic excitations in NaOsO through its metal-insulator transition
- High-order Dy multipole motifs observed in DyB2C2 with resonant soft x-ray Bragg diffraction
- Crossover from itinerant to localized magnetic excitations through the metal-insulator transition in NaOsO
- Crystal Symmetry Lowering in Chiral Multiferroic BaTaFeSiO observed by X-Ray Magnetic Scattering
Cited by in corpus (4)
- Lone octupole and bulk magnetism in osmate 5d2 double perovskites
- Study of polycrystalline bulk SrOsO double-perovskite insulator: comparison with 1000 K ferromagnetic epitaxial films
- Melting of magnetic order in by fs laser pulses
- Altermagnetism and Weak Magnetism in the Insulating Distorted Perovskite Antiferromagnet NaOsO