4.5 Article

Topological Protection and Control of Quantum Markovianity

Journal

PHOTONICS
Volume 7, Issue 1, Pages -

Publisher

MDPI
DOI: 10.3390/photonics7010018

Keywords

decoherence dynamics; topological order; Anderson localization; quantum-Hall topological insulators; non-Markovianity in open quantum systems

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Funding

  1. CAIB postdoctoral program
  2. Maria de Maetzu Program for Units of Excellence in RD [MDM-2017-0711]

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Under the Born-Markov approximation, a qubit system, such as a two-level atom, is known to undergo a memoryless decay of quantum coherence or excitation when weakly coupled to a featureless environment. Recently, it has been shown that unavoidable disorder in the environment is responsible for non-Markovian effects and information backflow from the environment into the system owing to Anderson localization. This turns disorder into a resource for enhancing non-Markovianity in the system-environment dynamics, which could be of relevance in cavity quantum electrodynamics. Here we consider the decoherence dynamics of a qubit weakly coupled to a two-dimensional bath with a nontrivial topological phase, such as a two-level atom embedded in a two-dimensional coupled-cavity array with a synthetic gauge field realizing a quantum-Hall bath, and show that Markovianity is protected against moderate disorder owing to the robustness of chiral edge modes in the quantum-Hall bath. Interestingly, switching off the gauge field, i.e., flipping the bath into a topological trivial phase, allows one to re-introduce non-Markovian effects. Such a result indicates that changing the topological phase of a bath by a tunable synthetic gauge field can be harnessed to control non-Markovian effects and quantum information backflow in a qubit-environment system.

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