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arXiv:2403.07866 · Physical review. B./Physical review. B

Robustness of a state with Ising topological order against local projective measurements

Sanjeev Kumar, Vikram Tripathi

Published Oct 22, 2024• 0 citations
arXivHTMLPDF

Abstract

We investigate the fragility of quantum information in a topologically ordered state, namely, the ground state of a weakly Zeeman perturbed honeycomb Kitaev model under unitary (Hamiltonian) evolution interrupted by random local projective measurements of the spins, using the tripartite mutual information $\ensuremath{\gamma}$---equivalent to the topological entanglement entropy for topologically ordered states---as a measure. Our findings show that in the steady state, $\ensuremath{\gamma}$ remains significant up to high measurement rates per site $r$ comparable to the Kitaev coupling scale when the initial state has Ising topological order (ITO), beyond which it degrades with increasing $r.$ We contrast this with the Abelian ${Z}_{2}$ topologically ordered ground state in the toric code regime of the Kitaev model with the same energy per site, which has garnered greater attention in the literature of fault-tolerant quantum computation. We observe that $\ensuremath{\gamma}$ in the toric code regime of the Kitaev model collapses rapidly beyond very small values of $r.$ Further, we also find that at high measurement rates, while topological order is lost, certain observables leave distinct signatures of the initial quantum state, thus providing a diagnostic of the topological order.

DOI
10.1103/physrevb.110.l161111

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We investigate the fragility of quantum information in a topologically ordered state, namely, the ground state of a weakly Zeeman perturbed honeycomb Kitaev model under unitary (Hamiltonian) evolution interrupted by random local projective measurements of the spins, using the tripartite mutual information \ensuremathγ\ensuremath{\gamma}\ensuremathγ---equivalent to the topological entanglement entropy for topologically ordered states---as a measure. Our findings show that in the steady state, \ensuremathγ\ensuremath{\gamma}\ensuremathγ remains significant up to high measurement rates per site rrr comparable to the Kitaev coupling scale when the initial state has Ising topological order (ITO), beyond which it degrades with increasing r.r.r. We contrast this with the Abelian Z2{Z}_{2}Z2​ topologically ordered ground state in the toric code regime of the Kitaev model with the same energy per site, which has garnered greater attention in the literature of fault-tolerant quantum computation. We observe that \ensuremathγ\ensuremath{\gamma}\ensuremathγ in the toric code regime of the Kitaev model collapses rapidly beyond very small values of r.r.r. Further, we also find that at high measurement rates, while topological order is lost, certain observables leave distinct signatures of the initial quantum state, thus providing a diagnostic of the topological order.
The topological order of the Kitaev toric code is insensitive to disorder in its couplings since all star and plaquette operators commute; consequently, the stabilizer ground-state manifold is independent of the individual coupling strengths, and the phase remains stable against weak local perturbations. This insensitivity, however, is a property of the eigenstates and not of the dynamics they generate, and we show that the disorder sensitivity of a probe prepared outside that eigenbasis can be a metrological resource. In particular, we investigate the estimation of the strength of three topological-order-breaking perturbations, the nonlinear Castelnovo-Chamon deformation, nearest-neighbor Ising interactions, and a magnetic field along horizontal edges, encoded on an initially separable probe through unitary evolution under the disordered toric code Hamiltonian. We demonstrate that the quenched average quantum Fisher information (QFI), a figure of merit for metrological precision, exceeds that of its ordered counterpart in suitable regimes of perturbation strength and encoding time. For the ordered case, we further identify optimal product probes, for which the quadratic and cubic terms of the short-time expansion vanish identically, leaving a transient quartic scaling of QFI. Interestingly, this window persists as long as the multipartite entanglement generated by the encoding continues to increase, and it survives under local dephasing, bit-flip, and amplitude damping noise acting independently on each site, with the non-unital channel being the least detrimental.
Kitaev's honeycomb model is a paradigmatic exactly solvable system hosting a quantum spin liquid with non-Abelian anyons and topologically protected edge modes, offering a platform for fault-tolerant quantum computation. However, real candidate Kitaev materials invariably include complex secondary interactions that obscure the realization of spin-liquid behavior and demand novel quantum computational approaches for efficient simulation. Here we report quantum simulations of a 22-site Kitaev honeycomb lattice on a trapped-ion quantum processor, without and with non-integrable Heisenberg interactions that are present in real materials. We develop efficient quantum circuits for ground-state preparation, achieving high accuracy with energy errors equivalent to an effective temperature of 0.2 (in units of the Kitaev interactions), consistent with the experimentally relevant spin-liquid regime. Starting from these states, we apply controlled perturbations and measure time-dependent spin correlations along the system's edge. In the non-Abelian phase, we observe chiral edge dynamics consistent with a non-zero Chern number, a hallmark of topological order, which vanishes upon transition to the Abelian toric code phase. Extending to the non-integrable Kitaev-Heisenberg model, we find that weak Heisenberg interactions preserve chiral edge dynamics, while stronger couplings suppress them, signaling the breakdown of topological protection. Our work demonstrates a viable route for probing dynamical signatures of topological order in quantum spin liquids using programmable quantum hardware, opening new pathways for quantum simulation of strongly correlated materials.
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Abstract The Kitaev honeycomb model is an approximate topological quantum error correcting code in the same phase as the toric code, but requiring only a 2-body Hamiltonian. As a frustrated spin model, it is well outside the commuting models of topological quantum codes that are typically studied, but its exact solubility makes it more amenable to analysis of effects arising in this noncommutative setting than a generic topologically ordered Hamiltonian. Here we study quantum error correction in the honeycomb model using both analytic and numerical techniques. We first prove explicit exponential bounds on the approximate degeneracy, local indistinguishability, and correctability of the code space. These bounds are tighter than can be achieved using known general properties of topological phases. Our proofs are specialized to the honeycomb model, but some of the methods may nonetheless be of broader interest. Following this, we numerically study noise caused by thermalization processes in the perturbative regime close to the toric code renormalization group fixed point. The appearance of non-topological excitations in this setting has no significant effect on the error correction properties of the honeycomb model in the regimes we study. Although the behavior of this model is found to be qualitatively similar to that of the standard toric code in most regimes, we find numerical evidence of an interesting effect in the low-temperature, finite-size regime where a preferred lattice direction emerges and anyon diffusion is geometrically constrained. We expect this effect to yield an improvement in the scaling of the lifetime with system size as compared to the standard toric code.
We present a method of extracting information about the topological order from the ground state of a strongly correlated two-dimensional system computed with the infinite projected entangled pair state (iPEPS). For topologically ordered systems, the iPEPS wrapped on a torus becomes a superposition of degenerate, locally indistinguishable ground states. Projectors in the form of infinite matrix product operators onto states with well-defined anyon flux are used to compute topological SSS and TTT matrices (encoding mutual and self-statistics of emergent anyons). The algorithm is shown to be robust against a perturbation driving string-net toric code across a phase transition to a ferromagnetic phase. Our approach provides accurate results near quantum phase transition, where the correlation length is prohibitively large for other numerical methods. Moreover, we used numerically optimized iPEPS describing the ground state of the Kitaev honeycomb model in the toric code phase and obtained topological data in excellent agreement with theoretical prediction.
We demonstrate that multipartite entanglement, witnessed by the quantum Fisher information, can characterize topological quantum phase transitions in the spin-12\frac{1}{2}21​ toric code model (TCM) on a square lattice with external fields. We show that the quantum Fisher information density of the ground state can be written in terms of the expectation values of gauge-invariant Wilson loops for different sizes of square regions and identify Z2{\mathbb{Z}}_{2}Z2​ topological order by its scaling behavior. Furthermore, we use this multipartite entanglement witness to investigate thermalization and disorder-assisted stabilization of topological order after a quantum quench. Moreover, with an upper bound of the quantum Fisher information, we demonstrate the absence of finite-temperature topological order in the two-dimensional TCM in the thermodynamic limit. Our results provide insights to topological phases, which are robust against external disturbances and are candidates for topologically protected quantum computation.