Abstract

Recently, rutile ${\mathrm{RuO}}_{2}$ has raised interest for its itinerant antiferromagnetism, crystal Hall effect, and strain-induced superconductivity. Understanding and manipulating these properties demands resolving the electronic structure and the relative roles of the rutile crystal field and $4d$ spin-orbit coupling (SOC). Here, we use O-K and Ru ${M}_{3}$ x-ray absorption and Ru ${M}_{3}$ resonant inelastic x-ray scattering to disentangle the contributions of crystal field, SOC, and electronic correlations in ${\mathrm{RuO}}_{2}$. The locally orthorhombic site symmetry of the Ru ions introduces significant crystal field contributions beyond the approximate octahedral coordination yielding a crystal field energy scale of $\mathrm{\ensuremath{\Delta}}({t}_{2g})\ensuremath{\approx}1\phantom{\rule{0.16em}{0ex}}\mathrm{eV}$ breaking the degeneracy of the ${t}_{2g}$ orbitals. This splitting exceeds the Ru SOC ($\ensuremath{\approx}160$ meV) suggesting a more subtle role of SOC, primarily through the modification of itinerant (rather than local) $4d$ electronic states, ultimately highlighting the importance of the local symmetry in ${\mathrm{RuO}}_{2}$. Remarkably, our analysis can be extended to other members of the rutile family, thus advancing the comprehension of the interplay among crystal field symmetry, electron correlations, and SOC in transition metal compounds with the rutile structure.

Highlights

  • Transition metal dioxides of the rutile structure exhibit many paradigmatic electronic phenomena arising from the delicate balance of strong electron correlations and spin-orbit coupling (SOC)

  • We find a low sensitivity of the x-ray absorption spectroscopy (XAS) or RIXS spectra to the intermediate state pd correlation scaling, which is due to the larger relative intermediate-state spin-orbit splitting between the 4d M2,3 edges compared to 3d TM L2,3 edges [55]

  • This characteristic mixture of localized or itinerant electronic states may lead to a spectrum of partial excitations, where the emission stage of the coherent RIXS process is only active from the dx2−y2 state, which forms a sharp peak in the occupied density of states [16]

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Summary

INTRODUCTION

Transition metal dioxides of the rutile structure exhibit many paradigmatic electronic phenomena arising from the delicate balance of strong electron correlations and spin-orbit coupling (SOC). A few examples include the metal-insulator transition in VO2 [1,2,3,4], the half-metallic ferromagnetism of CrO2 [5], and the SOC-mediated spin Hall effect in IrO2 [6,7,8] Many of these phenomena stem from the unique rutile structural symmetry, wherein transition metal sites of orthorhombic (D2h) site symmetry are coordinated to distorted oxygen octahedra, forming a bonding network with mixed edge- and corner-sharing octahedral configurations. Our combined experimental evidence and crystal field multiplet (CFM) simulations underscore the dominant role of lower-symmetry (below Oh) crystal field splitting [ (t2g) ≈ 1 eV] over the 4d SOC (160 meV), which has the effect of breaking the t2g degeneracy This defines how the orbital and band degeneracies are lifted from a high-symmetry coordination due to structural rather than relativistic effects, marking important constraints to explain the unconventional properties in RuO2.

EXPERIMENT
MODELING
D2h symmetry
Interpretation of crystal field parameters
Implications for RuO2
Findings
Comparison among metallic states in rutile oxides
CONCLUSION
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