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Topological Phase Transitions (BKT)

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Free Vortices
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Bound Pairs
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Phase
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T / T_BKT
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Berezinskii-Kosterlitz-Thouless (BKT) Transition

The BKT transition is a topological phase transition in 2D systems (e.g. thin film superfluids, XY spin model). Below T_BKT, vortex-antivortex pairs are bound and the system shows quasi-long-range order. Above T_BKT, pairs unbind and free vortices proliferate, destroying order.

Free energy: F = (E - TS) ≈ (π J - 2T) ln(R/a)
Helicity modulus jump: ΔΥ(T_BKT) = 2T_BKT/π (Nelson-Kosterlitz)

Vortex winding number n = ±1. The interaction energy between a vortex pair separated by r is E ≈ 2πJ ln(r/a). Free vortices screen this logarithmic interaction, producing exponential correlation decay.

This transition earned Kosterlitz and Thouless the 2016 Nobel Prize in Physics.