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通过控制正交双色场之间的相位来选择高次谐波产生中的轨迹。

Trajectory selection in high harmonic generation by controlling the phase between orthogonal two-color fields.

机构信息

Blackett Laboratory, Imperial College London, Prince Consort Road, London SW7 2BW, United Kingdom.

出版信息

Phys Rev Lett. 2011 Oct 7;107(15):153902. doi: 10.1103/PhysRevLett.107.153902.

Abstract

We demonstrate control of short and long quantum trajectories in high harmonic emission through the use of an orthogonally polarized two-color field. By controlling the relative phase ϕ between the two fields we show via classical and quantum calculations that we can steer the two-dimensional trajectories to return, or not, to the core and so control the relative strength of the short or long quantum trajectory contribution. In experiments, we demonstrate that this leads to robust control over the trajectory contributions using a drive field from a femtosecond laser composed of the fundamental ω at 800 nm (intensity ∼1.2×10(14)  W cm(-2)) and its weaker orthogonally polarized second harmonic 2ω (intensity ∼0.3×10(14)  W cm(-2)) with the relative phase between the ω and 2ω fields varied simply by tilting a fused silica plate. This is the first demonstration of short and long quantum trajectory control at the single-atom level.

摘要

我们通过使用正交偏振双色场演示了在高次谐波发射中对短和长量子轨迹的控制。通过控制两个场之间的相对相位 ϕ,我们通过经典和量子计算表明,我们可以引导二维轨迹返回核心,或者不返回核心,从而控制短或长量子轨迹贡献的相对强度。在实验中,我们通过使用由基频 ω 在 800nm(强度约为 1.2×10(14)  W cm(-2)) 和其较弱的正交偏振二次谐波 2ω(强度约为 0.3×10(14)  W cm(-2))组成的飞秒激光产生的驱动场,演示了这种控制对轨迹贡献的强大控制,其中 ω 和 2ω 场之间的相对相位通过简单地倾斜熔融石英板来改变。这是在单原子水平上首次演示短和长量子轨迹控制。

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