Abstract

A self-correcting quantum memory can store and protect quantum information for a time that increases without bound with the system size and without the need for active error correction. We demonstrate that symmetry can lead to self-correction in 3D spin-lattice models. In particular, we investigate codes given by 2D symmetry-enriched topological (SET) phases that appear naturally on the boundary of 3D symmetry-protected topological (SPT) phases. We find that while conventional on-site symmetries are not sufficient to allow for self-correction in commuting Hamiltonian models of this form, a generalized type of symmetry known as a 1-form symmetry is enough to guarantee self-correction. We illustrate this fact with the 3D "cluster-state" model from the theory of quantum computing. This model is a self-correcting memory, where information is encoded in a 2D SET-ordered phase on the boundary that is protected by the thermally stable SPT ordering of the bulk. We also investigate the gauge color code in this context. Finally, noting that a 1-form symmetry is a very strong constraint, we argue that topologically ordered systems can possess emergent 1-form symmetries, i.e., models where the symmetry appears naturally, without needing to be enforced externally.

Highlights

  • Quantum-error-correcting codes can be used to protect information in a noisy quantum computer

  • A self-correcting quantum memory (SCQM) in d spatial dimensions is a quantum-manybody spin system with the following four properties: (i) The Hilbert space consists of a finite density of finite-dimensional spins in d spatial dimensions; (ii) the Hamiltonian H has local terms with bounded strength and range, such that each spin is in the support of only a constant number of terms; (iii) the ground space of H is degenerate such that a qubit can be encoded in the ground space and that this ground space is perturbatively stable; (iv) the lifetime of the stored information after coupling the system to a thermal bath must grow without bound in the system size

  • We show that spin-lattice models corresponding to 2D symmetry-enriched topological (SET)-ordered boundaries of thermally stable 3D SPTordered phases protected by a suitable 1-form symmetry can be self-correcting quantum memories

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Summary

INTRODUCTION

Quantum-error-correcting codes can be used to protect information in a noisy quantum computer. The four-dimensional generalization of the toric code [1] provides a canonical example of a self-correcting quantum memory. Symmetry can provide new directions in the search for self-correcting quantum memories, as the landscape of ordered spin-lattice models becomes even richer when one considers the interplay of symmetry and topology. We show that a self-correcting quantum memory can be encoded in a 2D SET boundary of this 3D model, and it is protected by the thermally stable SPT ordering of the bulk. We discuss the possibility of such 1-form symmetries being emergent in 3D topological models in Sec. V based around the gauge color code.

Self-correcting quantum memories
Thermalization and memory time
Energy barrier
Dimensionality of excitations and self-correction
Topological phases with symmetry
Symmetry-protected topological phases
Symmetry-enriched topological phases
Higher-form symmetries
Self-correction and topological order
Symmetry constraints and quantum memories
No spontaneous symmetry breaking
On-site symmetries are insufficient for stability
System-bath coupling with symmetry and the symmetric energy barrier
SELF-CORRECTION WITH A 1-FORM SPT PHASE
The RBH bulk Hamiltonian
Bulk excitations without symmetry
Bulk excitations with 1-form symmetries
Boundaries I
Boundary condensation
Boundaries II
Boundary degrees of freedom
Symmetry action on the boundary
Toric code boundary Hamiltonian
Toric code boundary excitations
Energetics of boundary excitations
Comparison
Boundaries III
Primal boundary
Dual boundary
Sink boundary
The lattice
The Hamiltonian
The ground space
Logical operators and code space
Logical operator decomposition
The energy barrier
Self-correction
Encoding with more general topologies
Topological obstruction to logical decompositions
Bulk boundary correspondence at nonzero temperature
THE GAUGE COLOR CODE PROTECTED BY 1-FORM SYMMETRY
Subsystem codes
The gauge color code lattice
The 3D gauge color code
A commuting model
Relation to the RBH model
EMERGENT 1-FORM SYMMETRIES
Emergent 0-form symmetries in 2D
Single-sector 3D gauge color code
The gauge color code and color flux conservation
Higher-dimensional generalizations and emergent q-form symmetries
Stability of emergent symmetries
We label ground states of H by jψii and ground states of
Duality between emergent and enforceable symmetries
DISCUSSION
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