Abstract

We investigate the possibility to control quantum evolution speed of a single dephasing qubit for arbitrary initial states by the use of periodic dynamical decoupling (PDD) pulses. It is indicated that the quantum speed limit time (QSLT) is determined by initial and final quantum coherence of the qubit, as well as the non-Markovianity of the system under consideration during the evolution when the qubit is subjected to a zero-temperature Ohmic-like dephasing reservoir. It is shown that final quantum coherence of the qubit and the non-Markovianity of the system can be modulated by PDD pulses. Our results show that for arbitrary initial states of the dephasing qubit with non-vanishing quantum coherence, PDD pulses can be used to induce potential acceleration of the quantum evolution in the short-time regime, while PDD pulses can lead to potential speedup and slow down in the long-time regime. We demonstrate that the effect of PDD on the QSLT for the Ohmic or sub-Ohmic spectrum (Markovian reservoir) is much different from that for the super-Ohmic spectrum (non-Markovian reservoir).

Highlights

  • We present a proposal to manipulate the quantum evolution speed of qubits in an open system for arbitrary initial states by employing periodic dynamical decoupling (PDD) pulses[43]

  • Unlike previous results for qubits in amplitude damping channel[41] or in X-Y spin-chain environment[42], in this paper we investigate the influence of PDD pulse sequences on the QSLT of the qubit in a pure dephasing reservoir in both short- and long-time regimes for arbitrary initial states

  • Our findings show that the QSLT of a dephasing qubit under PDD pulses is determined by the initial and final quantum coherence of the qubit, as well as the non-Markovianity of the system during the evolution

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Summary

Introduction

We present a proposal to manipulate the quantum evolution speed of qubits in an open system for arbitrary initial states by employing periodic dynamical decoupling (PDD) pulses[43]. Our findings show that the QSLT of a dephasing qubit under PDD pulses is determined by the initial and final quantum coherence of the qubit, as well as the non-Markovianity of the system during the evolution.

Results
Conclusion

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