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Reentrant Localization in Quasiperiodic Thue-Morse Chain

Taylan Yildiz, B. Tanatar

Abstract

We investigate localization and reentrance in a dimerized Su-Schrieffer-Heeger (SSH) tight-binding chain whose on-site energies are given by a quasiperiodic cosine masked by a deterministic Thue-Morse sequence. Working with non-interacting, spinless fermions, we solve the model via exact diagonalization on large Fibonacci sizes and diagnose phases using inverse/normalized participation ratios and the correlation fractal dimension. We identify boundaries separating extended, multifractal (mixed), and localized regimes by constructing a phase diagram in the plane of modulation strength and dimerization ratio. As the quasiperiodic amplitude is increased, the system exhibits reentrant behavior, localizing, partially re-delocalizing into a multifractal regime, and re-localizing, verified via two-size crossings of band-averaged observables and finite-size scaling. We demonstrate that tuning the modulation strength, the SSH dimerization, or the incommensurability parameter provides control over the critical thresholds. Our results suggest a versatile, randomness-free platform for the deterministic control of transport, enabling switching between conducting, multifractal, and insulating states.

Reentrant Localization in Quasiperiodic Thue-Morse Chain

Abstract

We investigate localization and reentrance in a dimerized Su-Schrieffer-Heeger (SSH) tight-binding chain whose on-site energies are given by a quasiperiodic cosine masked by a deterministic Thue-Morse sequence. Working with non-interacting, spinless fermions, we solve the model via exact diagonalization on large Fibonacci sizes and diagnose phases using inverse/normalized participation ratios and the correlation fractal dimension. We identify boundaries separating extended, multifractal (mixed), and localized regimes by constructing a phase diagram in the plane of modulation strength and dimerization ratio. As the quasiperiodic amplitude is increased, the system exhibits reentrant behavior, localizing, partially re-delocalizing into a multifractal regime, and re-localizing, verified via two-size crossings of band-averaged observables and finite-size scaling. We demonstrate that tuning the modulation strength, the SSH dimerization, or the incommensurability parameter provides control over the critical thresholds. Our results suggest a versatile, randomness-free platform for the deterministic control of transport, enabling switching between conducting, multifractal, and insulating states.
Paper Structure (8 sections, 19 equations, 12 figures)

This paper contains 8 sections, 19 equations, 12 figures.

Figures (12)

  • Figure 1: Illustration of the model described with $3$ unit cells and with length $6$ Thue-Morse sequence
  • Figure 2: Real-space profiles of the middle eigenstate $\psi_i$ (eigen-index $m/L=0.5$) for four potential strengths $\delta=0,\,0.6,\,1.1,$ and $3.0$. Parameters: system size $N=2584$, $J_2=0.7$.
  • Figure 3: Density plot of fractal dimension $D_2$ with respect to eigenstate index with the system size 1597 and with 20 different box sizes
  • Figure 4: Averaged fractal dimension $D_2$ over the middle of the spectrum with respect to $\delta$ for $N=1597,2584,4181,6765$ and extrapolated result for $N\rightarrow\infty$.
  • Figure 5: Average IPR and NPR with respect to potential strength $\delta$ for states in the middle of the spectra and for system size $L=13530$, shaded regions correspond to critical phases. (a) for $J_2=0.7$ (b) for $J_2=1.2$
  • ...and 7 more figures