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The real- space interpretation of Eq.3 can be found in End Matter

The three AFM states are described by ( ⃗J1, ⃗J2) = ( S1+S2 2 , S1−S2 2 ) = J(ˆx, ˆx), J(ˆx, 0), J(ˆx, ˆy)

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Odd-parity Magnetism Driven by Antiferromagnetic Exchange

cond-mat.str-el · 2025-01-03 · accept · novelty 7.0

Coplanar antiferromagnetic order in non-symmorphic crystals can induce odd-parity spin splitting, nematic order, or scalar odd-parity order, with microscopic models and 67 material candidates identified.

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  • Odd-parity Magnetism Driven by Antiferromagnetic Exchange cond-mat.str-el · 2025-01-03 · accept · none · ref 1

    Coplanar antiferromagnetic order in non-symmorphic crystals can induce odd-parity spin splitting, nematic order, or scalar odd-parity order, with microscopic models and 67 material candidates identified.