Topological invariants for interacting systems: From twisted boundary conditions to center-of-mass momentum

Beyond the well-known topological band theory for single-particle systems, it is a great challenge to char-acterize the topological nature of interacting multiparticle quantum systems. Here, we uncover the relation between topological invariants defined through the twisted boundary condition (TBC) and the center-of-mass (c.m.) momentum state in multiparticle systems. We find that the Berry phase defined through the TBC can be equivalently obtained from the multiparticle Wilson loop formulated by c.m. momentum states. As the Chern number can be written as the winding of the Berry phase, we consequently prove the equivalence of Chern numbers obtained via TBC and c.m. momentum state approaches. As a proof-of-principle example, we study topological properties of the Aubry-Andre-Harper model. Our numerical results show that the TBC approach and c.m. approach are well consistent with each other for both the many-body case and the few-body case. Our work lays a concrete foundation and provides insights for exploring multiparticle topological states.

Automated summary

Beyond the well-known topological band theory for single-particle systems, it is a great challenge to characterize the topological nature of interacting multiparticle quantum systems. Here, we uncover the relationship between topological invariants defined through the twisted boundary condition (TBC) and the center-of-mass (c.m.) momentum state in multiparticle systems. Our work lays a concrete foundation and provides insights for exploring multiparticle topological states.