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氦的强场激发:束缚态分布与自旋效应。

Strong-field excitation of helium: bound state distribution and spin effects.

作者信息

Zimmermann H, Buller J, Eilzer S, Eichmann U

机构信息

Max-Born-Institute, Max-Born-Straße 2a, 12489 Berlin, Germany.

Institut für Optik und Atomare Physik, Technische Universität Berlin, 10623 Berlin, Germany.

出版信息

Phys Rev Lett. 2015 Mar 27;114(12):123003. doi: 10.1103/PhysRevLett.114.123003. Epub 2015 Mar 24.

Abstract

Using field ionization combined with the direct detection of excited neutral atoms we measured the distribution of principal quantum number n of excited He Rydberg states after strong-field excitation at laser intensities well in the tunneling regime. Our results confirm theoretical predictions from semiclassical and quantum mechanical calculations and simultaneously underpin the validity of the semiclassical frustrated tunneling ionization model. Moreover, since our experimental detection scheme is spin sensitive in the case of He atoms, we show that strong-field excitation leads to strong population of triplet states. The origin of it lies in the fact that high angular momentum states are accessible in strong-field excitation. Thus, singlet-triplet transitions become possible due to the increased importance of spin-orbit interaction rather than due to direct laser induced spin-flip processes.

摘要

利用场电离结合对激发态中性原子的直接探测,我们测量了在隧道电离区域的激光强度下强场激发后氦里德堡激发态主量子数(n)的分布。我们的结果证实了半经典和量子力学计算的理论预测,同时支持了半经典受挫隧道电离模型的有效性。此外,由于我们的实验探测方案对氦原子的情况具有自旋敏感性,我们表明强场激发导致三重态的大量出现。其根源在于在强场激发中高角动量态是可及的。因此,单重态 - 三重态跃迁成为可能是由于自旋 - 轨道相互作用重要性的增加,而非由于直接的激光诱导自旋翻转过程。

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