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Home/Chemistry/Anderson Localization (1D Tight-Binding)

Anderson Localization (1D Tight-Binding)

Random onsite disorder W on a 1-D chain: diagonalize H, plot |ψ|² eigenstates, IPR vs energy, and localization length estimates (RMS and exponential fit).

Tight-binding chain

80
3
1
40

Open 1-D Anderson model H = −t Σ|c†_i c_{i+1}| + h.c. + Σ ε_i n_i with ε_i uniform on [−W/2, W/2]. Exact diagonalization gives eigenstates ψ and energies E. IPR = Σ|ψ_i|⁴ is small (~1/N) for extended states and large for localized ones. Pink bars: IPR > 5/N heuristic.

Measured values

Energy E-0.0131
IPR0.1972
Extended IPR ≈ 1/N0.0125
RMS extent3.15 sites
ξ (exp. fit)7.3 sites
Disorder W3.00

About this model

Anderson localization explains why electronic (or wave) eigenstates in a disordered crystal can remain spatially confined even when the underlying lattice supports propagation. This simulator implements the standard 1-D tight-binding Anderson Hamiltonian on an open chain: H = −t Σ_i (|i⟩⟨i+1| + h.c.) + Σ_i ε_i |i⟩⟨i| with hopping amplitude t and independent random onsite energies ε_i drawn uniformly from [−W/2, W/2]. The disorder strength W is measured in units of t. The full N×N matrix is diagonalized numerically to obtain eigenenergies E_n and eigenvectors ψ_n. For each state you can inspect the probability density |ψ_i|² along the chain, the onsite disorder landscape ε_i, and the inverse participation ratio IPR = Σ_i |ψ_i|⁴ — small (of order 1/N) for delocalized band states and large for localized states. A scatter plot of IPR versus E highlights how states near the band center localize as W increases, while the clean chain (W = 0) recovers extended Bloch-like eigenstates. Localization length is estimated two ways: the RMS spatial extent of |ψ|² and an exponential fit of ln|ψ| to distance from the peak amplitude. Finite chain length and open boundaries are important caveats: edge reflections and level repulsion modify the spectrum compared with an infinite system, but the IPR diagnostic remains the standard classroom measure of localization.

Who it's for: Graduate or advanced undergraduate solid-state physics students studying disordered systems, after band structure and before scaling/localization length concepts in 2D/3D.

Key terms

  • Anderson localization
  • Tight-binding model
  • Disorder potential
  • Inverse participation ratio
  • Localization length
  • Eigenstate
  • Density of states

How it works

Anderson localization in a 1-D tight-binding chain with random onsite disorder: eigenstates, |ψ|² profiles, inverse participation ratio, and localization length estimates — the standard condensed-matter disorder demo.

Frequently asked questions

What does the disorder parameter W mean?
Each site energy ε_i is uniform on [−W/2, W/2]. W = 0 is a perfect chain with bandwidth 4t. Increasing W broadens the spectrum and tends to localize states in the band center in 1D; W is always quoted in the same units as the hopping t (here t = 1 by default).
How should I read the IPR?
With normalized ψ, IPR = Σ|ψ_i|⁴. For a state spread over all N sites with comparable amplitude, IPR ~ 1/N. For a state confined to a few sites, IPR approaches O(1). The dashed reference line marks 1/N on the IPR–energy plot.
Why do pink bars appear on |ψ|²?
They mark states with IPR > 5/N, a simple heuristic for “more localized than a uniformly extended state” on this finite chain. It is a visualization aid, not a rigorous critical criterion.
Is there a mobility edge in 1D?
For the 1-D Anderson model with site disorder, essentially all eigenstates are localized for any W > 0 in the infinite-system limit. Mobility edges appear in higher dimensions; this page is intentionally 1D to show eigenvectors and IPR directly.