Perturbative stability and error correction thresholds of quantum codes

TL;DR

This paper links topological stability and quantum error correction by constructing classical models for decoding and analyzing phase transitions, providing insights into the stability thresholds of quantum codes under perturbations.

Contribution

It introduces a unified framework connecting classical statistical mechanics models with quantum code stability, including proofs of phase existence and error correction success probabilities.

Findings

Existence of low-temperature ordered phases for certain quantum codes.

Success probabilities bound order parameters in lattice gauge theories.

Evidence for stable phases in perturbed quantum Hamiltonians.

Abstract

Topologically-ordered phases are stable to local perturbations, and topological quantum error-correcting codes enjoy thresholds to local errors. We connect the two notions of stability by constructing classical statistical mechanics models for decoding general CSS codes and classical linear codes. Our construction encodes correction success probabilities under uncorrelated bit-flip and phase-flip errors, and simultaneously describes a generalized Z2 lattice gauge theory with quenched disorder. We observe that the clean limit of the latter is precisely the discretized imaginary time path integral of the corresponding quantum code Hamiltonian when the errors are turned into a perturbative X or Z magnetic field. Motivated by error correction considerations, we define general order parameters for all such generalized Z2 lattice gauge theories, and show that they are generally lower bounded by success probabilities of error correction. For CSS codes satisfying the LDPC condition and with a sufficiently large code distance, we prove the existence of a low temperature ordered phase of the corresponding lattice gauge theories, particularly for those lacking Euclidean spatial locality and/or when there is a nonzero code rate. We further argue that these results provide evidence to stable phases in the corresponding perturbed quantum Hamiltonians, obtained in the limit of continuous imaginary time. To do so, we distinguish space- and time-like defects in the lattice gauge theory. A high free-energy cost of space-like defects corresponds to a successful "memory experiment" and suppresses the energy splitting among the ground states, while a high free-energy cost of time-like defects corresponds to a successful "stability experiment" and points to a nonzero gap to local excitations.