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arXiv · 1511.05854

Biexponential decay and ultralong coherence of a single qubit

Jérôme Flakowski·Maksym Osmanov·David Taj·Hans Christian Öttinger
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Abstract

A quantum two-state system, weakly coupled to a heat bath, is traditionally studied in the Born-Markov regime under the secular approximation with completely positive linear master equations. Despite its success, this microscopic approach exclusively predicts exponential decays and Lorentzian susceptibility profiles, in disagreement with a number of experimental findings. To leave this limited paradigm, we use a phenomenological positive nonlinear master equation being both thermodynamically and statistically consistent. We find that, beyond a temperature-dependent threshold, a bifurcation in the decoherence time $T_2$ takes place; it gives rise to a biexponential decay and a susceptibility profile being neither Gaussian nor Lorentzian. This implies that, for suitable initial states, a major prolongation of the coherence can be obtained in agreement with recent experiments. Moreover, $T_2$ is no longer limited by the energy relaxation time $T_1$ offering novel perspectives to elaborate devices for quantum information processing.

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Jérôme Flakowski, Maksym Osmanov, David Taj, Hans Christian Öttinger. 2015-11-18. Biexponential decay and ultralong coherence of a single qubit. https://doi.org/10.1209/0295-5075%2F113%2F40003

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