For square lattice and weakly deformed square lattice bulk media with a magnetic domain wall, the band gap is traversed by two edge-state eigenvalue curves seeded by effective matrix Schrödinger and Dirac edge Hamiltonians.
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Edge states in square lattice media and their deformations
For square lattice and weakly deformed square lattice bulk media with a magnetic domain wall, the band gap is traversed by two edge-state eigenvalue curves seeded by effective matrix Schrödinger and Dirac edge Hamiltonians.