Orbital ferromagnetism in graphene
We break the I and TR symmetries in single-layer graphene by introducing the mass term (M) and next nearest neighbor hopping term (\(t_2\)) (as discussed in Sec. Tight-binding Hamiltonain). This results in…
We break the I and TR symmetries in single-layer graphene by introducing the mass term (M) and next nearest neighbor hopping term (\(t_2\)) (as discussed in Sec. Tight-binding Hamiltonain). This results in…