Fermionic approach to variational quantum simulation of Kitaev spin models
arXiv:2204.05322 · doi:10.1103/PhysRevA.106.022434
Abstract
We use the variational quantum eigensolver (VQE) to simulate Kitaev spin models with and without integrability breaking perturbations, focusing in particular on the honeycomb and square-octagon lattices. These models are well known for being exactly solvable in a certain parameter regime via a mapping to free fermions. We use classical simulations to explore a novel variational ansatz that takes advantage of this fermionic representation and is capable of expressing the exact ground state in the solvable limit. We also demonstrate that this ansatz can be extended beyond this limit to provide excellent accuracy when compared to other VQE approaches. In certain cases, this fermionic representation is advantageous because it reduces by a factor of two the number of qubits required to perform the simulation. We also comment on the implications of our results for simulating non-Abelian anyons on quantum computers.
References in corpus (11)
- -RuCl3: a Spin-Orbit Assisted Mott Insulator on a Honeycomb Lattice
- On the Origin of Zigzag Magnetic Order in Iridium Oxide Na2IrO3
- Exact results for spin dynamics and fractionization in the Kitaev Model
- Possible proximity of the Mott insulating Iridate Na2IrO3 to a topological phase: Phase diagram of the Heisenberg-Kitaev model in a magnetic field
- Dynamically Generated Logical Qubits
- Efficient step-merged quantum imaginary time evolution algorithm for quantum chemistry
- Phase diagram and spin correlations of the Kitaev-Heisenberg model: Importance of quantum effects
- Probing the stability of the spin liquid phases in the Kitaev-Heisenberg model using tensor network algorithms
- Density-Matrix Renormalization Group Study of Extended Kitaev-Heisenberg Model
- A family of stabilizer codes for anyons and Majorana modes
- A quantum Monte Carlo method on asymptotic Lefschetz thimbles for quantum spin systems: An application to the Kitaev model in a magnetic field