The bond-disordered Kitaev model attracts much attention due to the experimental relevance in α-RuCl₃ and A₃LiIr₂O₆ (A = H, D, Ag, etc.). Applying a magnetic field to break the time-reversal symmetry leads to a strong modulation in mass terms for Dirac cones. Because of the smallness of the flux gap of the Kitaev model, a small bond disorder can have large influence on itinerant Majorana fermions. The quantization of the thermal Hall conductivity κ^xy/T disappears by a quantum Hall transition induced by a small disorder, and κ^xy/T shows a rapid crossover into a state with a negligible Hall current. We call this immobile liquid state Anderson–Kitaev spin liquid (AKSL). Especially, the critical disorder strength δJ_c1 ~ 0.05 in the unit of the Kitaev interaction would have many implications for the stability of Kitaev spin liquids.

由于在α- RuCl ₃和A ₃ LiIr ₂ O ₆（A = H，D，Ag等）中的实验相关性，无序的Kitaev模型引起了很多关注。施加磁场以破坏时间反转对称性会导致Dirac锥的质量调制变强。由于Kitaev模型的通量间隙较小，因此小的键合紊乱可能会对流动的Majorana费米子产生较大影响。热霍尔的量化电导率κ ^{X ý} / Ť通过一个小障碍引起的量子霍尔过渡消失，并且κ ^{X ÿ} / Ť显示了快速过渡到霍尔电流可忽略不计的状态。我们称这种不流动的液态安德森-基塔耶夫旋转液（AKSL）。特别是，临界病症强度δ Ĵ _C1在Kitaev相互作用的单元〜0.05会对的Kitaev自旋液体的稳定性的许多问题。