Recent lattice studies have revealed that the color flux tube between static quark–antiquark pairs exhibits an excess entanglement entropy (flux-tube entanglement entropy, FTE
2) that scales linearly with the quark separation
. In this paper, we demonstrate similar behavior in a
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Recent lattice studies have revealed that the color flux tube between static quark–antiquark pairs exhibits an excess entanglement entropy (flux-tube entanglement entropy, FTE
2) that scales linearly with the quark separation
. In this paper, we demonstrate similar behavior in a string-net model based on
fusion categories, where the nontrivial object
(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
objects using the microcanonical (equal-weight) prescription
and find an entropy density
. For
, the category reduces to the Fibonacci case, yielding an entropy density σ
3 = 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, minimizing the free energy
yields a confinement–deconfinement transition at
, which is first-order-like (tension sign reversal) rather than a continuous critical transition. The parameter
offers a tunable knob, making the
family a computable 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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