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    Magnetic circular dichroism in core-level x-ray photoelectron spectroscopy of altermagnetic RuO2 films

    Y. Lytvynenko1,2, A. Akashdeep1, T. P. Vo3,4, O. Tkach1,5, S. V. Chernov6, A. Gloskovskii6, C. Schlueter6, C. Luo7, V. Ukleev7 et al.

    F. Radu7, F. Kronast7, T. Hiroto8, A. Winkelmann9, J. Minár3, M. Kläui1, G. Schönhense1, G. Jakob1, H. J. Elmers1,*, and O. Fedchenko1,10

    • *Contact author: elmers@uni-mainz.de

    Phys. Rev. B 113, 014403 – Published 5 January, 2026

    DOI: https://doi.org/10.1103/x2h4-rtky

    Abstract

    While ferromagnetism and antiferromagnetism are well-established classes of magnetic order, a third class of collinear magnetic order, termed altermagnetism, has recently attracted scientific interest. We measured magnetic circular dichroism (MCD) in core-level photoemission (XPS) at the Ru 2p3/2 and 2p1/2 core levels in epitaxial RuO2(110)/TiO2(110) films using circularly polarized x rays at 6 keV, as well as x-ray magnetic circular dichroism (XMCD) in resonant x-ray absorption at the Ru M3,2 (3p3/2 and 3p1/2) edges. Charge transfer multiplet calculations show that the MCD-XPS and the XMCD can be explained by an altermagnetic locking of Ru magnetic moments and a distorted crystal field orientation. The distortion is caused by the epitaxial strain. The collinear magnetic moments in RuO2 occupy sublattice sites with distorted octahedral crystal fields that are rotated by 90∘ with respect to each other. A change in the sign of the MCD-XPS at different sample positions indicates the presence of altermagnetic domains with the size of around hundreds of micrometers.

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