Reentrant localization transition induced by a composite potential

We numerically investigate the localization transition in a one-dimensional system subjected to a composite potential consisting of periodic and quasiperiodic components. For the rational wave vector $\ensuremath{\alpha}=1/2$, the periodic component reduces to a staggered potential, which has been reported to induce the reentrant localization transition. In addition to $\ensuremath{\alpha}=1/2$, we find that other rational wave vectors can also lead to the reentrant phenomenon. To investigate the underlying mechanisms of the reentrant localization transition, we vary the parameters of the composite potential and find that the reentrant localization transition is sensitive to the phase factor of the periodic component. By further studying the structure of the periodic component, we confirm that this sensitivity arises from the periodic phase factor modulating the mirror symmetry. Finally, we map out a global phase diagram and reveal that the reentrant localization transition originates from a paradoxical effect: Increasing the amplitude of the periodic component enhances localization but simultaneously strengthens the mirror symmetry, which favors the formation of extended states. Our numerical analysis suggests that the interplay between these competing factors drives the reentrant localization transition.