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Theoretical study demonstrates linear flux-tube entanglement entropy scaling in SU(2)k string-net models, highlighting a tunable platform for entropic confinement in quantum simulators.
Recent lattice studies have revealed that the color flux tube between static quark–anti-quark pairs exhibits an excess entanglement entropy (flux-tube entanglement entropy, FTE2) that scales linearly with the quark separation L. In this paper, we demonstrate sim-ilar behavior in a string-net model based on SU(2)k fusion categories, where the nontriv-ial object j = 1/2 (analogous to color charge) cannot exist in isolation due to the fusion rules, naturally exhibiting “confinement”. We compute the entanglement entropy of the flux tube connecting two j = 1/2 objects using the microcanonical (equal-weight) pre-scription S(R) = ln(dim(Hom(R))) and find an entropy density σk = ln d1/2 = ln(2cos\({π/k+2}\)). For 𝑘 = 3, the category reduces to the Fibonacci case, yielding an entropy density σ3 = ln φ ≈ 0.4812 (φ is the golden ratio), which is qualitatively comparable in magnitude to the scale inferred from lattice studies and the entropy surface mechanism. Under a thermalization assumption for the fusion-channel degrees of freedom, minimiz-ing the free energy F = (𝒥 \({-}\) Tσk)L yields a confinement–deconfinement transition at (Tc = 𝒥/σk), which is first-order-like (tension sign reversal) rather than a continuous crit-ical transition. The parameter k offers a tunable knob, making the SU(2)k family a com-putable laboratory for entropic confinement. The predicted entropy-density jump can be directly tested in quantum simulator platforms (e.g., Rydberg arrays or superconducting circuits) that realize Fibonacci anyonic models.
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Xiaodong Yang (2026) studied this question.
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