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arXiv:1302.3428 · Reviews of Modern Physics

Quantum error correction for quantum memories

Barbara M. Terhal

Published Apr 7, 2015• 1,351 citations
arXivHTMLPDF

Abstract

It may seem inevitable that highly entangled quantum states are susceptible to disturbance through interaction with a decohering environment. However, certain multiqubit entangled states are well protected from common forms of decoherence as the quantum information is hidden in inherently nonlocal degrees of freedom. This review shows that this robustness is enabled by specific measurements on subsets of qubits, implementing a quantum version of an error correction process. Beginning with the basics, the latest understanding of the relation between this form of error correction and the concept of two-dimensional topological order in many-body physics is reviewed.

DOI
10.1103/revmodphys.87.307

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The field of quantum computing holds immense promise for solving complex problems that are currently intractable for classical computers. However, the practical realization of quantum computers faces a critical challenge: the inherent fragility of qubits, the fundamental units of quantum information. Quantum systems are susceptible to various types of errors and decoherence due to their interaction with the surrounding environment, which can lead to a rapid degradation of quantum information. This chapter delves into the pivotal aspect of quantum error correction techniques as a means to mitigate the adverse effects of errors and decoherence in quantum computing systems. Begins by elucidating the theoretical foundations of quantum error correction, exploring the principles that underlie the encoding of quantum information into larger, redundant codes that are resilient to errors. A comprehensive overview of prominent quantum error correction codes, such as the stabilizer codes and topological codes, is provided, along with a discussion of their respective strengths and limitations.
Quantum error correction is a set of methods to protect quantum information--that is, quantum states--from unwanted environmental interactions (decoherence) and other forms of noise. The information is stored in a quantum error-correcting code, which is a subspace in a larger Hilbert space. This code is designed so that the most common errors move the state into an error space orthogonal to the original code space while preserving the information in the state. It is possible to determine whether an error has occurred by a suitable measurement and to apply a unitary correction that returns the state to the code space, without measuring (and hence disturbing) the protected state itself. In general, codewords of a quantum code are entangled states. No code that stores information can protect against all possible errors; instead, codes are designed to correct a specific error set, which should be chosen to match the most likely types of noise. An error set is represented by a set of operators that can multiply the codeword state. Quantum error correction is used to protect information in quantum communication (where quantum states pass through noisy channels) and quantum computation (where quantum states are transformed through a sequence of imperfect computational steps in the presence of environmental decoherence to solve a computational problem). In quantum computation, error correction is just one component of fault-tolerant design.
Quantum error correction is a set of methods to protect quantum information--that is, quantum states--from unwanted environmental interactions (decoherence) and other forms of noise. The information is stored in a quantum error-correcting code, which is a subspace in a larger Hilbert space. This code is designed so that the most common errors move the state into an error space orthogonal to the original code space while preserving the information in the state. It is possible to determine whether an error has occurred by a suitable measurement and to apply a unitary correction that returns the state to the code space, without measuring (and hence disturbing) the protected state itself. In general, codewords of a quantum code are entangled states. No code that stores information can protect against all possible errors; instead, codes are designed to correct a specific error set, which should be chosen to match the most likely types of noise. An error set is represented by a set of operators that can multiply the codeword state. Quantum error correction is used to protect information in quantum communication (where quantum states pass through noisy channels) and quantum computation (where quantum states are transformed through a sequence of imperfect computational steps in the presence of environmental decoherence to solve a computational problem). In quantum computation, error correction is just one component of fault-tolerant design.
Quantum information theory stands at a critical juncture, grappling with the challenges of maintaining quantum coherence in the face of inevitable noise. Current error correction methods, while effective, are fundamentally limited by the complexity of encoding and decoding processes. This paper proposes a novel approach to quantum error correction centered around the concept of topological quantum information, exploring the potential to encode quantum information within the inherent structure of spacetime. This fundamentally shifts the paradigm away from traditional error-correcting codes and towards a more robust and potentially universal approach. The core mechanism involves developing a 'topological field' encoding scheme inspired by topological insulators, aiming to create inherently robust quantum states resistant to local perturbations. We will detail the theoretical framework, the implementation challenges, and preliminary experimental considerations for this approach. The core claim is that this novel methodology offers a path towards significantly enhanced quantum information protection.
All physical systems that provide a good template for the implementation of qubits and quantum gates suffer from some degree of decoherence. The reason is simple: no physical system exists in complete isolation; if it did exist, it would be useless for quantum computing since you would not be able to interact with it! Any physical system, even when well protected, will eventually interact with its environment in a way that we cannot predict or completely control. As a result, coherence, which is essential for quantum information processing, is progressively lost. In the field of quantum computation, it was realized early on that strategies must be employed to mitigate not only imprecisions in the instrumentation but also errors associated to decoherence and relaxation due to interactions with the environment. These strategies, when employed at the quantum circuit level, are called quantum error correction (QEC).