Quantized Thouless pumps with paths containing the noninteracting singularity

Determine whether quantized Thouless pumps can be observed in interacting one-dimensional systems even when the closed adiabatic path includes the noninteracting topological singularity at (J'/J = 1, Δ = 0) of the Rice–Mele limit.

Background

Thouless pumps provide a dynamical probe of topology in one-dimensional systems, typically realized in the noninteracting Rice–Mele model by adiabatically encircling the singular point (J'/J = 1, Δ = 0) while maintaining a finite gap through symmetry breaking. Interactions are known to modify or even break quantized pumping, for instance via emergent Mott physics, although interaction-enabled or quasiquantized pumps have also been reported under certain conditions.

Previous works have considered displaced paths that avoid the noninteracting singularity or rely on finite-size gaps. The question of whether quantized pumping can persist when the periodic path actually contains the noninteracting singularity—particularly in the thermodynamic limit—had not been explicitly settled.

References

An open question is whether quantized Thouless pumps can be observed in interacting systems, in the extreme case where the periodic adiabatic path contains the noninteracting topological singularity.

Quantized Thouless pumps protected by interactions in dimerized Rydberg tweezer arrays  (2402.09311 - Julià-Farré et al., 2024) in Introduction