Twisted double- and mono-bilayer graphene are graphene-based moiré
materials hosting strongly correlated fermions in a gate-tunable
conduction band with a topologically non-trivial character. Using
unbiased exact diagonalization complemented by unrestricted Hartree-Fock
calculations, we find that the strong electron-electron interactions
lead to a non-coplanar magnetic state, which has the same symmetries as
the tetrahedral antiferromagnet on the triangular lattice and can be
thought of as a skyrmion lattice commensurate with the moiré scale,
competing with a set of ferromagnetic, topological charge density waves
featuring an approximate emergent O(3) symmetry, “rotating” the
different charge density wave states into each other. Direct comparison
with exact diagonalization reveals that the ordered phases are
accurately described within the unrestricted Hartree-Fock approximation.
Exhibiting a finite charge gap and Chern number
|C|=1,
the formation of charge density wave order which is intimately connected
to a skyrmion lattice phase is consistent with recent experiments on
these systems.