Twisted bilayer graphene near the magic angle is known to have a cascade of insulating phases at integer filling factors of the low-energy bands. In this Letter we address the nature of these phases through an unrestricted, large-scale Hartree-Fock calculation on the lattice that self-consistently accounts for all electronic bands. Using numerically unbiased methods, we show that Coulomb interactions produce ferromagnetic insulating states at integer fillings $\nu \in [-3,3]$ with maximal spin polarization $M_{\text{FM}}=4-\left|\nu \right|$. We find that the $\nu =0$ state is a pure ferromagnet, whereas all other insulating states are spin-valley polarized. At odd filling factors $\left|\nu \right|=1,3$ those states have a quantum anomalous Hall effect with Chern number $\mathcal{C}=1$. Except for the $\nu =0,-2$ states, all other integer fillings have insulating phases with additional sublattice symmetry breaking and antiferromagnetism in the remote bands. We map the metal-insulator transitions of these phases as a function of the effective dielectric constant. Our results establish the importance of large-scale lattice calculations to faithfully determine the ground states of twisted bilayer graphene at integer fillings.

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• Quantum many-body systems
• Topological materials
• Twisted heterostructures
• Electron-correlation calculations
• Many-body techniques
• Tight-binding model