Abstract

The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evolve between two states. For open quantum systems this quantity depends on the dynamical map describing the time evolution in presence of the environment, on the evolution time τ, and on the initial state of the system. We consider a general single qubit open dynamics and show that there is no simple relationship between memory effects and the tightness of the QSL bound. We prove that only for specific classes of dynamical evolutions and initial states, there exists a link between non-Markovianity and the QSL. Our results shed light on the connection between information back-flow between system and environment and the speed of quantum evolution.

Highlights

  • The idea of the possible existence of a fundamental limit, dictated by the principles of quantum mechanics, for the speed of evolution of quantum states was firstly discussed in [1]

  • Our main goal is to tackle the question of the connection between non-Markovianity and the quantum speed limit (QSL) not starting from a specific model but in full generality, looking in detail at the role played by the dynamical map, the evolution time τ, and the initial state, in the achievement of the QSL bound

  • We have studied the connection between the QSL, the evolution time, non-Markovianity, and the initial state for a qubit system undergoing generic and several large subclasses of dynamics

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Summary

17 December 2019

The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to. For open quantum systems this quantity depends on the dynamical map this work must maintain attribution to the describing the time evolution in presence of the environment, on the evolution time τ, and on the author(s) and the title of initial state of the system. We consider a general single qubit open dynamics and show that there is no the work, journal citation and DOI. Simple relationship between memory effects and the tightness of the QSL bound. We prove that only for specific classes of dynamical evolutions and initial states, there exists a link between non-. Our results shed light on the connection between information back-flow between system and environment and the speed of quantum evolution

Introduction
Damped JC model
Evolution time dependence of tQSL t
Connection between BLP non-Markovianity and QSL
Pairwise oscillating translation and deformation
Unital maps
Example: phase-covariant commutative dynamics
Initial state dependence of QSL for Markovian master equations
Phase-covariant
Eternal non-Markovianity
The effect of Markovian-to-non-Markovian transition in QSL time
Conclusions
Full Text
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