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2D XY model: BKT vortex unbinding

What you are seeing: a 2D grid where each site holds an angle (a "compass needle") that can point anywhere from 0 to 360 degrees. Neighbors prefer to point in the same direction (E=Jcos(θiθj)E = -J\cos(\theta_i - \theta_j) per bond). At low TT all needles align approximately; at high TT they go random. The interesting feature: the transition is not a sharp ordering but a Kosterlitz- Thouless transition where pairs of vortices (rotational defects) unbind.

Each cell is colored by the angle (rainbow modulo 2π2\pi). Red and blue dots mark +2π+2\pi and 2π-2\pi vortices, found by computing the winding number around each plaquette. The transition temperature is TBKT0.893JT_\text{BKT} \approx 0.893 J; below it vortices pair up; above it they roam free. Watch the vortex count climb past TBKTT_\text{BKT}.

Figure 1. 2D XY model angles colored by direction; vortices marked by colored dots. Method: single-spin Metropolis.
T0.70
L64
speed3

WHAT TO TRY

  • Vary each control and watch the rail readouts respond.
  • Compare the diagnostic plot against the live scene.