Extended Data Fig. 9: Kagome lattice model.
From: Giant and anisotropic many-body spin–orbit tunability in a strongly correlated kagome magnet
a, Kagome lattice with Kane–Mele SOI. Here, \({v}_{{\rm{A}}{\rm{B}}}=2({{\boldsymbol{d}}}_{1}\times {{\boldsymbol{d}}}_{2})\cdot {\boldsymbol{z}}/\sqrt{3}=-1\), where d1 is the unit vector from A to C and d2 is the unit vector from C to B. b, Flux Ω enclosed by the fundamental plaquette formed by sites A, B and C on the kagome lattice.
