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arxiv: 1411.6643 · v4 · pith:DJMOXEWGnew · submitted 2014-11-24 · 🪐 quant-ph · cond-mat.stat-mech· cond-mat.str-el

Quantum memories at finite temperature

classification 🪐 quant-ph cond-mat.stat-mechcond-mat.str-el
keywords quantummemoriesfinitepassiveseveraltemperaturetheoremsactive
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To use quantum systems for technological applications we first need to preserve their coherence for macroscopic timescales, even at finite temperature. Quantum error correction has made it possible to actively correct errors that affect a quantum memory. An attractive scenario is the construction of passive storage of quantum information with minimal active support. Indeed, passive protection is the basis of robust and scalable classical technology, physically realized in the form of the transistor and the ferromagnetic hard disk. The discovery of an analogous quantum system is a challenging open problem, plagued with a variety of no-go theorems. Several approaches have been devised to overcome these theorems by taking advantage of their loopholes. Here we review the state-of-the-art developments in this field in an informative and pedagogical way. We give the main principles of self-correcting quantum memories and we analyze several milestone examples from the literature of two-, three- and higher-dimensional quantum memories.

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Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Mixed-state topological order and the errorfield double formulation of decoherence-induced transitions

    quant-ph 2023-01 unverdicted novelty 6.0

    Decoherence on abelian topological order is modeled as a temporal defect in double TQFT driving boundary anyon condensation transitions classified by Lagrangian subgroups of the doubled order.