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高标度频率下里德堡原子微波电离的量子抑制

Quantum suppression of microwave ionization of Rydberg atoms at high scaled frequency.

作者信息

Maeda H, Gallagher T F

机构信息

Department of Physics, University of Virginia, Charlottesville, Virginia 22904-0714, USA.

出版信息

Phys Rev Lett. 2004 Nov 5;93(19):193002. doi: 10.1103/PhysRevLett.93.193002. Epub 2004 Nov 4.

Abstract

Microwave ionization of Rydberg atoms is well described as the onset of classical chaos when the microwave frequency omega is less than the Kepler frequency 1/n(3). However, when omega>1/n(3), i.e., at high scaled frequency Omega=omegan(3)>1, classical ionization is predicted to be suppressed by quantum interference, an analogue to Anderson localization in a solid. Using 17.55 GHz microwave fields we have observed the ionization of Sr Rydberg atoms in the regime 1</=Omega</=5 . Our measurements demonstrate the quantum suppression of classical diffusive ionization and show the ionization field to be n independent in this regime.

摘要

当微波频率ω小于开普勒频率1/n³时,里德伯原子的微波电离被很好地描述为经典混沌的开始。然而,当ω>1/n³时,即在高标度频率Ω = ωn³>1时,经典电离预计会被量子干涉抑制,这类似于固体中的安德森局域化。我们使用17.55 GHz的微波场,在1≤Ω≤5的范围内观测到了锶里德伯原子的电离。我们的测量结果证明了经典扩散电离的量子抑制,并表明在该范围内电离场与n无关。

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