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dc.contributor.authorJheng, Shih-Daen_US
dc.contributor.authorJiang, Tsin-Fuen_US
dc.contributor.authorChen, Jen-Haoen_US
dc.contributor.authorLiu, Jinn-Liangen_US
dc.date.accessioned2018-08-21T05:53:51Z-
dc.date.available2018-08-21T05:53:51Z-
dc.date.issued2018-08-01en_US
dc.identifier.issn0031-8949en_US
dc.identifier.urihttp://dx.doi.org/10.1088/1402-4896/aaca08en_US
dc.identifier.urihttp://hdl.handle.net/11536/145252-
dc.description.abstractPhotoelectron spectra and transition mechanisms of a hydrogen atom in the n = 2 state under circularly polarized pulses in the barrier suppression ionization (BSI) regime, found by solving the time-dependent Schrodinger equation, are presented in detail. The photoelectron peak emerges from low-energy, in contrast to being centered at higher energy in the case of ionization from the ground state. We show that the magnetic quantum number dependence of photoelectron angular distributions on initial states yields 3- and 2-band structures for 2p(-) and 2p(0) in zenith angle, respectively, and 1-band structures for both 2p(+) and 2s. The intermediate transition pathways from these initial states to the corresponding final states are also revealed.en_US
dc.language.isoen_USen_US
dc.subjectbarrier suppression ionizationen_US
dc.subjectcircularly polarized pulseen_US
dc.subjectphotoelectron angular distributionen_US
dc.subjecttransition mechanismen_US
dc.titleMagnetic quantum number dependence of hydrogen photoelectron spectra under circularly polarized pulse in barrier suppression ionization regimeen_US
dc.typeArticleen_US
dc.identifier.doi10.1088/1402-4896/aaca08en_US
dc.identifier.journalPHYSICA SCRIPTAen_US
dc.citation.volume93en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000438486600001en_US
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