Infinite-Randomness Fixed Points for Chains of Non-Abelian Quasiparticles

Abstract

One-dimensional chains of non-Abelian quasiparticles described by $SU(2{)}_k$ Chern-Simons-Witten theory can enter random singlet phases analogous to that of a random chain of ordinary spin-1/2 particles (corresponding to $k\to \infty$). For $k=2$ this phase provides a random singlet description of the infinite randomness fixed point of the critical transverse field Ising model. The entanglement entropy of a region of size $L$ in these phases scales as $S_L\simeq \frac{\ln d}{3}{\log }_{2}L$ for large $L$, where $d$ is the quantum dimension of the particles.

4 pages, 4 figures

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