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Dynamics of a two-level system under strong driving: quantum gate optimization based on floquet theory

机译:强驱动下两级系统的动力学:量子门   基于Floquet理论的优化

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摘要

We consider the dynamics of a two-level system (qubit) driven by strong andshort resonant pulses in the framework of Floquet theory. First we deriveanalytical expressions for the quasienergies and Floquet states of the drivensystem. If the pulse amplitude varies very slowly, the system adiabaticallyfollows the instantaneous Floquet states, which acquire dynamical phases thatdepend on the evolution of the quasienergies over time. The difference betweenthe phases acquired by the two Floquet states corresponds to a qubit staterotation, generalizing the notion of Rabi oscillations to the case of largedriving amplitudes. If the pulse amplitude changes very fast, the evolution isnon-adiabatic, with transitions taking place between the Floquet states. Wequantify and analyze the nonadiabatic transitions during the pulse by employingadiabatic perturbation theory and exact numerical simulations. We find that,for certain combinations of pulse rise and fall times and maximum drivingamplitude, a destructive interference effect leads to a remarkably strongsuppression of transitions between the Floquet states. This effect provides thebasis of a quantum control protocol, which we name Floquet InterferenceEfficient Suppression of Transitions in the Adiabatic basis (FIESTA), that canbe used to design ultra-fast high-fidelity single-qubit quantum gates.
机译:我们在Floquet理论的框架内考虑由强和短共振脉冲驱动的两级系统(qubit)的动力学。首先,我们得出驱动系统的准能量和浮球状态的解析表达式。如果脉冲幅度变化非常缓慢,则系统将绝热地遵循瞬时Floquet状态,该状态将获得依赖于准能量随时间变化的动态相位。由两个浮球状态获得的相位之间的差异对应于量子比特状态旋转,从而将拉比振荡的概念推广到大的驱动幅度的情况下。如果脉冲幅度变化非常快,则演化是非绝热的,并且在浮球状态之间发生过渡。通过采用绝热微扰理论和精确的数值模拟,对脉冲中的非绝热跃迁进行量化和分析。我们发现,对于脉冲上升和下降时间以及最大驱动振幅的某些组合,相消干涉效应会明显抑制Floquet状态之间的跃迁。这种效应提供了量子控制协议的基础,我们将其称为绝热基础上的浮子干扰有效抑制跃迁(FIESTA),可用于设计超快速高保真单量子位量子门。

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