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A theoretical study on the strong-field ionization of the lithium atom

dc.citation.epageen_US
dc.citation.issue11en_US
dc.citation.volume46en_US
dc.citation.woscount2
dc.contributor.authorJheng, Shih-Daen_US
dc.contributor.authorJiang, T. F.en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.date.accessioned2014-12-08T15:30:35Z
dc.date.available2014-12-08T15:30:35Z
dc.date.issued2013-06-14en_US
dc.description.abstractWe apply a recently developed momentum space method (Jiang et al 2012 Phys. Rev. E 86 066702) to investigate the experimental results of strong-field ionization of the lithium atom (Schuricke et al 2011 Phys. Rev. A 83 023413). By splitting the photoelectron into groups of even and odd angular momenta and by using the states' population history, we can analyse the ionization mechanism in further detail. The lower energy double-peak structure, shown experimentally, of the photoelectron is attributed to the three-level Lambda-coupling effect. The spectral difference of 10 and 30 fs pulses at a typical intensity is demonstrated. We explain why the strong-field ionization fluctuates at intensities of 6 and 10 fs, but not for a 30 fs pulse. The change of fan-like photoelectron angular distribution with intensity in direction parallel to polarization is explained. Use of the Keldysh parameter to classify the tunnelling and multiphoton ionization is not meaningful for the lithium atom, because the ground state is mostly depleted before reaching peak intensity.en_US
dc.identifier.doi10.1088/0953-4075/46/11/115601en_US
dc.identifier.issn0953-4075en_US
dc.identifier.journalJOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICSen_US
dc.identifier.urihttp://dx.doi.org/10.1088/0953-4075/46/11/115601en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/21851
dc.identifier.wosnumberWOS:000319122200016
dc.language.isoen_USen_US
dc.titleA theoretical study on the strong-field ionization of the lithium atomen_US
dc.typeArticleen_US

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