We investigate numerically how on-site disorder affects conduction in the periodically driven Rice-Mele model, a prototypical realization of the Thouless pump. Although the pump is robust against disorder in the fully adiabatic limit, much less is known about the case of finite period time $T$, which is relevant also in light of recent experimental realizations. We find that, at any fixed period time and nonzero disorder, increasing the system size $L\to \infty$ always leads to a breakdown of the pump, indicating Anderson localization of the Floquet states. Our numerics indicate, however, that, in a properly defined thermodynamic limit, where $L/T^{\theta }$ is kept constant, Anderson localization can be avoided, and the charge pumped per cycle has a well-defined value — as long as the disorder is not too strong. The critical exponent $\theta$ is not universal, rather, its value depends on the disorder strength. Our findings are relevant for practical, experimental realizations of the Thouless pump, for studies investigating the nature of its current-carrying Floquet eigenstates, as well as the mechanism of the full breakdown of the pump, expected if the disorder exceeds a critical value.

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• Anderson localization
• Symmetry protected topological states
• Topological insulators
• Topological phases of matter
• 1-dimensional systems
• Quantum many-body systems
• Bloch-Floquet theorem
• Exact diagonalization
• Exact solutions for many-body systems