Disorder, Low-Energy Excitations, and Topology in the Kitaev Spin Liquid

The Kitaev model is a fascinating example of an exactly solvable model displaying a spin-liquid ground state in two dimensions. However, deviations from the original Kitaev model are expected to appear in real materials. In this Letter, we investigate the fate of Kitaev???s spin liquid in the presence of disorder???bond defects or vacancies???for an extended version of the model. Considering static flux backgrounds, we observe a power-law divergence in the low-energy limit of the density of states with a nonuniversal exponent. We link this power-law distribution of energy scales to weakly coupled droplets inside the bulk, in an uncanny similarity to the Griffiths phase often present in the vicinity of disordered quantum phase transitions. If time-reversal symmetry is broken, we find that power-law singularities are tied to the destruction of the topological phase of the Kitaev model in the presence of bond disorder alone. However, there is a transition from this topologically trivial phase with power-law singularities to a topologically nontrivial one for weak to moderate site dilution. Therefore, diluted Kitaev materials are potential candidates to host Kitaev???s chiral spin-liquid phase.

Automated summary

Investigated the fate of Kitaev's spin liquid in the presence of disorder in an extended version of the model. Found a power-law divergence in the low-energy limit of the density of states, similar to the Griffiths phase. Power-law singularities are tied to the destruction of the topological phase of the Kitaev model in the presence of bond disorder, but a transition to a topologically nontrivial phase is possible for weak to moderate site dilution.