Two-body interactions cause charge pumping to lose quantization in the driven Falicov-Kimball model despite persisting edge modes, due to interaction-induced broadening, with distinct energy dissipation rates in high- versus intermediate-frequency regimes.
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Effect of Two-Body Interactions on Floquet topological phases
Two-body interactions cause charge pumping to lose quantization in the driven Falicov-Kimball model despite persisting edge modes, due to interaction-induced broadening, with distinct energy dissipation rates in high- versus intermediate-frequency regimes.