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Nonrelativistic spin splitting has emerged as a defining feature of unconventional magnetic states. Here we show that quantum interference offers a symmetry-resolved probe for the parity of such spin splitting, as even- and odd-parity magnets exhibit qualitatively different weak (anti-)localization behaviors. Even-parity magnets can host time-reversal symmetric scattering loops depicted by the spin group, giving rise to a weak localization that can be suppressed by spin-orbit coupling. In contrast, odd-parity magnets have a hidden weak antilocalization that can be released by spinorbit coupling. We further derive the corresponding magnetoconductivity formulas to facilitate experimental explorations. Our results not only advance the weak (anti-)localization theory to unconventional magnets but also suggest a practical diagnostic of unconventional spin-split magnetic states.
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Chen et al. (2026) studied this question.
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