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Second, notice that the residues of the poles atu=ξandu=−ik 1 vanish upon antisymmetrization

(S75) × A σ(k3 −iξ) Z d2ue − 1 2 u2+ i 2 (u¯k1−¯uk1)¯σ(k1 −iu)σ(k 2 −iu) σ(k2 −k 1 +i(u−ξ)) σ(k2 −k 1)σ(i(u−ξ)) =e i 2 (¯k3+¯k2−¯k1)ξe− 1 4 (k2 1+k2 2+k2 3) Z d2ue − 1 2 u2+ i 2 (u

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Microsopic Theory of Spin Polarons in Chern Ferromagnets

cond-mat.str-el · 2026-05-06 · accept · novelty 7.0

Closed-form wavefunctions for charge-e spin polarons in SU(2) Chern ferromagnets are exact eigenstates in ideal Chern-1 bands with contact interactions and remain stable variational states when quantum geometry is controlled.

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  • Microsopic Theory of Spin Polarons in Chern Ferromagnets cond-mat.str-el · 2026-05-06 · accept · none · ref 62

    Closed-form wavefunctions for charge-e spin polarons in SU(2) Chern ferromagnets are exact eigenstates in ideal Chern-1 bands with contact interactions and remain stable variational states when quantum geometry is controlled.