2018
DOI: 10.1103/physrevb.98.245148
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Topological charge pumping in the interacting bosonic Rice-Mele model

Abstract: We investigate topological charge pumping in a system of interacting bosons in the tight-binding limit, described by the Rice-Mele model. An appropriate topological invariant for the many-body case is the change of polarization per pump cycle, which we compute for various interaction strengths from infinite-size matrix-product-state simulations. We verify that the charge pumping remains quantized as long as the pump cycle avoids the superfluid phase. In the limit of hardcore bosons, the quantized pumped charge… Show more

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Cited by 63 publications
(62 citation statements)
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“…As discussed by Hayward et al [31], the charge pumping in the RM model may as well be visualized by the evolution of the entanglement spectrum λ μ . In Fig.…”
Section: B Pair Pumpingmentioning
confidence: 98%
See 1 more Smart Citation
“…As discussed by Hayward et al [31], the charge pumping in the RM model may as well be visualized by the evolution of the entanglement spectrum λ μ . In Fig.…”
Section: B Pair Pumpingmentioning
confidence: 98%
“…This concept was first introduced by Thouless [25] and may be studied by the generalization of the SSH to the Rice-Mele (RM) model [26]. Recently, with the observation of charge pumping in cold-atom experiments [4][5][6][7], the fate of Thouless pumping in interacting systems, such as the interacting fermionic or bosonic RM model, has attracted a great deal of interest [27][28][29][30][31][32][33].…”
Section: Introductionmentioning
confidence: 99%
“…For interacting system, the topological pumping of two interacting bosons [7] and many-body case [35,36] has been investigated. However, these interacting models have the topological single-particle counterpart in the interaction-free condition.…”
Section: Interaction-induced Thouless Pumpingmentioning
confidence: 99%
“…For large enough |∆| and |t2 − t1|, a gapped Mott insulating (MI) phase is realized, while for small |∆| or |t2 − t1| the system is superfluid (SF), see (b). By adiabatically changing ∆ as well as t1 and t2 along a loop within the MI phase (parametrization ϕ, solid blue in (b)) a topological Thouless pump can be realized [68] which is characterized by a many body Chern number. To measure this Chern number directly we couple a hole excitation of the MI to a two-component impurity in a conventional lattice, leading to the formation of a topological polaron (TP).…”
Section: A Modelmentioning
confidence: 99%