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A no-go theorem for a two-dimensional self-correcting quantum memory based on stabilizer codes

TLDR
It is shown that for D=1,2 the height of the energy barrier separating different logical states is upper bounded by a constant independent of the lattice size L, and it is demonstrated that a self-correcting quantum memory cannot be built using stabilizer codes in dimensions D= 1,2.
Abstract
We study properties of stabilizer codes that permit a local description on a regular D-dimensional lattice. Specifically, we assume that the stabilizer group of a code (the gauge group for subsystem codes) can be generated by local Pauli operators such that the support of any generator is bounded by a hypercube of constant size. Our first result concerns the optimal scaling of the distance $d$ with the linear size of the lattice $L$. We prove an upper bound $d=O(L^{D-1})$ which is tight for D=1,2. This bound applies to both subspace and subsystem stabilizer codes. Secondly, we analyze the suitability of stabilizer codes for building a self-correcting quantum memory. Any stabilizer code with geometrically local generators can be naturally transformed to a local Hamiltonian penalizing states that violate the stabilizer condition. A degenerate ground-state of this Hamiltonian corresponds to the logical subspace of the code. We prove that for D=1,2 the height of the energy barrier separating different logical states is upper bounded by a constant independent of the lattice size L. The same result holds if there are unused logical qubits that are treated as "gauge qubits". It demonstrates that a self-correcting quantum memory cannot be built using stabilizer codes in dimensions D=1,2. This result is in sharp contrast with the existence of a classical self-correcting memory in the form of a two-dimensional ferromagnet. Our results leave open the possibility for a self-correcting quantum memory based on 2D subsystem codes or on 3D subspace or subsystem codes.

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Citations
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Quantum error correction for beginners.

TL;DR: The basic aspects of quantum error correction and fault-tolerance are examined largely through detailed examples, which are more relevant to experimentalists today and in the near future.
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Local stabilizer codes in three dimensions without string logical operators

TL;DR: It is proved that every stringlike logical operator of this code can be deformed to a disjoint union of short segments, each of which is in the stabilizer group, and introduced a notion of "logical string segments" to avoid difficulties in defining one-dimensional objects in discrete lattices.
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Holographic quantum error-correcting codes: Toy models for the bulk/boundary correspondence

TL;DR: In this article, a tensor network is proposed to capture key features of entanglement in the AdS/CFT correspondence, in particular the Ryu-Takayanagi formula and the negativity of tripartite information are obeyed exactly in many cases.
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Roads towards fault-tolerant universal quantum computation

TL;DR: In this article, the authors proposed a fault-tolerant logical qubit architecture for quantum computers, which uses high-dimensional quantum codes in a modular architecture, but need to be explored further.
References
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Journal ArticleDOI

Fault tolerant quantum computation by anyons

TL;DR: A two-dimensional quantum system with anyonic excitations can be considered as a quantum computer Unitary transformations can be performed by moving the excitations around each other Unitary transformation can be done by joining excitations in pairs and observing the result of fusion.
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Anyons in an exactly solved model and beyond

TL;DR: In this article, a spin-1/2 system on a honeycomb lattice is studied, where the interactions between nearest neighbors are of XX, YY or ZZ type, depending on the direction of the link; different types of interactions may differ in strength.
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Topological quantum memory

TL;DR: In this article, the authors studied the topological quantum error-correcting surface codes (surface codes) introduced by Kitaev, where qubits are arranged in a two-dimensional array on a surface of nontrivial topology.
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Markovian master equations

TL;DR: In this article, the memory effects in a quantum-mechanical master equation become negligible in the weak coupling limit for a finite-dimensional system weakly coupled to an infinite free heat bath.
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Topological quantum distillation.

TL;DR: These codes implement the whole Clifford group of unitary operations in a fully topological manner and without selective addressing of qubits, which allows them to extend their application also to quantum teleportation, dense coding, and computation with magic states.