In this work, we investigate the Kitaev honeycomb model employing the recently developed Clifford circuits augmented matrix product states (CAMPS) method. While the model in the gapped phase is known to reduce to the toric code model—whose ground state is entirely constructible from Clifford circuits—we demonstrate that the very different gapless quantum spin liquid (QSL) phase can also be significantly disentangled with Clifford circuits. Specifically, CAMPS simulations reveal that approximately two-thirds of the entanglement entropy in the isotropic point arises from Clifford-circuit contributions, enabling dramatically more efficient computations compared to conventional matrix product state (MPS) methods. Crucially, this finding implies that the Kitaev QSL state retains significant “Clifford-simulatable” structure, even in the gapless phase with non-Abelian anyon excitations when time reversal symmetry is broken. This property not only enhances classical simulation efficiency significantly but also suggests substantial resource reduction for preparing such states on quantum devices. As an application, we leverage CAMPS to study the Kitaev-Heisenberg model and determine the most accurate phase boundary between the antiferromagnetic phase and the Kitaev QSL phase in the model. Our results highlight how Clifford circuits can effectively disentangle the intricate entanglement of Kitaev QSLs, opening avenues for efficiently simulating related and similar strongly correlated models.

Close

PrevNext

View figure in article

• Quantum many-body systems
• Density matrix renormalization group
• Kitaev model
• Kitaev-Heisenberg model
• Matrix product states
• Tensor network methods