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      In the quest of relations between non-Markovianity and quantum optimal control

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          Abstract

          It is widely spread in the literature that non-Markovianity (NM) may be regarded as a resource in quantum mechanics. However, it is still unclear how and when this alleged resource may be exploited. Here, we study the relationship between NM and quantum optimal control in two paradigmatic non-Markovian systems, i.e. the spin star model and the Jaynes Cummings model. In both situations we find that the region of parameters in which both systems were originally more non-Markovian are compatible with the regions where the best control is achieved. Nevertheless, we show that non-Markovian effects are quite sensitive to the control field of the optimization, being able to increase or even decrease due to the latter. As a result, the degree of NM is actively manipulated by the field in order to improve the success of the protocol. Likewise, we finally show that where the system develops the largest degree of NM is at the same time where it becomes more controllable

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          Controlled dissociation of I2 via optical transitions between the X and B electronic states

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            Correlated projection operator approach to non-Markovian dynamics in spin baths

            The dynamics of an open quantum system is usually studied by performing a weak-coupling and weak-correlation expansion in the system-bath interaction. For systems exhibiting strong couplings and highly non-Markovian behavior this approach is not justified. We apply a recently proposed correlated projection superoperator technique to the model of a central spin coupled to a spin bath via full Heisenberg interaction. Analytical solutions to both the Nakajima-Zwanzig and the time-convolutionless master equation are determined and compared with the results of the exact solution. The correlated projection operator technique significantly improves the standard methods and can be applied to many physical problems such as the hyperfine interaction in a quantum dot.
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              Optimal control for non-Markovian open quantum systems

              An efficient optimal-control theory based on the Krotov method is introduced for a non-Markovian open quantum system with a time-nonlocal master equation in which the control parameter and the bath correlation function are correlated. This optimal-control method is developed via a quantum dissipation formulation that transforms the time-nonlocal master equation to a set of coupled linear time-local equations of motion in an extended auxiliary Liouville space. As an illustration, the optimal-control method is applied to find the control sequences for high-fidelity Z gates and identity gates of a qubit embedded in a non-Markovian bath. Z gates and identity gates with errors less than 10^{-5} for a wide range of bath decoherence parameters can be achieved for the non-Markovian open qubit system with control over only the {\sigma}z term. The control-dissipation correlation and the memory effect of the bath are crucial in achieving the high-fidelity gates.
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                Author and article information

                Journal
                28 November 2017
                Article
                1711.10551
                2e7a2642-8269-46d5-9330-49648d488562

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                9 pages, 5 figures
                quant-ph

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