pith. sign in

Hence, the symmetry operation{I sC −1 4z ||C4z}be- comes{I sC −1 4z ||KC4z} ≡T{C −1 4z ||C4z}, whereTis the time-reversal operation

The spin-only inversionI s is forced to become antiunitary (incorporating the complex conjugation operator K) in order to preserve the spin commutation relations when evaluated a

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Unconventional Mixed-Parity Magnetism in Rare-Earth Tetraborides

cond-mat.str-el · 2026-07-02 · unverdicted · novelty 7.0

TbB4 hosts component-resolved mixed-parity spin textures in a 3D compensated magnet, with p/f-wave odd parity in-plane and d-wave even parity out-of-plane, driven by staggered Berry phase from scalar spin chirality.

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  • Unconventional Mixed-Parity Magnetism in Rare-Earth Tetraborides cond-mat.str-el · 2026-07-02 · unverdicted · none · ref 60

    TbB4 hosts component-resolved mixed-parity spin textures in a 3D compensated magnet, with p/f-wave odd parity in-plane and d-wave even parity out-of-plane, driven by staggered Berry phase from scalar spin chirality.