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In this talk, we will show how the Ginsparg-Wilson relation can be generalized to boundary theories of various topological insulators and superconductors, emphasizing how perturbative and global anomalies arise naturally from the lattice measure. We will also discuss subtleties associated with a Hamiltonian formulation. Addressing these would be crucial for future quantum simulations of any quantum field theory where chiral symmetry plays an important role, such as QCD or the Standard Model.