pith. sign in

=⇒ −3|r− |λ||+ h 2u1 + 2 u2 + u3 4 i ρ2 = 0 =⇒ρ 2 = 3|r− |λ|| 2 u1 +u 2 + u3 4 (S6.8) where in the second step we have added the three equations

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Fluctuation-driven chiral ferromagnetism

cond-mat.str-el · 2026-05-07 · unverdicted · novelty 6.0

Quantum fluctuations stabilize a chiral ferromagnet with orbital chirality and a chiral stripe phase in the presence of magnetization-non-conserving spin-orbit interactions, producing an enhanced thermal Hall effect.

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  • Fluctuation-driven chiral ferromagnetism cond-mat.str-el · 2026-05-07 · unverdicted · none · ref 50

    Quantum fluctuations stabilize a chiral ferromagnet with orbital chirality and a chiral stripe phase in the presence of magnetization-non-conserving spin-orbit interactions, producing an enhanced thermal Hall effect.