Physic Labs

Condensed matter physics

Topological materials

Explore bulk energy bands and edge states in a topological insulator (SSH-style model). Observe how in-gap edge states appear and vanish as mass/disorder parameters change.

Research

Equipment

  • Bulk-band model and finite 1D chain with edges
  • Four sliders: mass m, symmetry disorder, model parameter, time
  • In-gap energy/state display and "Pause" button

Procedure

  1. Observe bulk bands and the gap

    In figure 1 "Bulk bands and edge states", see the two band branches and the gap between them. Set "Mass m" small: the gap closes — the system approaches a metal; increase m: the gap opens and edge states appear inside it, the topological character of the phase.

  2. Test the robustness of edge states

    With the gap open, raise the "Symmetry disorder" slider: the edge state survives until disorder is strong enough to close the gap — the signature of topological protection. In figure 2 "Spin and protecting symmetry", observe the spin–momentum locking of the edge state.

  3. Vary the model parameter and conclude

    Sweep "Model parameter" and "Time" to see the edge state propagate/localize at the boundary. Summarize the bulk–boundary rule: the bulk band's topological invariant (winding/Chern number) dictates the number of edge states that must exist — changing it requires closing the gap, i.e., a topological phase transition.

Simulation

Experiment history

Topological condensed-matter physics began with the integer quantum Hall effect (Klaus von Klitzing, 1980): the Hall conductance is quantized in exact multiples of e2/he^2/h, independent of sample details — later explained by Thouless, Kohmoto, Nightingale, and den Nijs (1982) via band Chern numbers. Su, Schrieffer, and Heeger (1979) had already built a polyacetylene chain model hosting edge states — now the canonical SSH model. In 2005–06 Kane–Mele and independently Bernevig–Hughes–Zhang predicted two-dimensional topological insulators with spin-locked edge channels; König confirmed them in HgTe quantum wells (2007). The 2016 Nobel Prize went to Thouless, Haldane, and Kosterlitz for topological phases of matter — opening the era of topological materials in the lab.

Related physicists

Related library topics