  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.
