首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Pump-probe photoelectron velocity-map imaging of autoionizing singly excited 4s~14p~6 np~1(n ~= 7,8)and doubly excited 4s~24p~45s~1 6p~1 resonances in atomic krypton
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Pump-probe photoelectron velocity-map imaging of autoionizing singly excited 4s~14p~6 np~1(n ~= 7,8)and doubly excited 4s~24p~45s~1 6p~1 resonances in atomic krypton

机译:自动激发原子k中的单激发4s〜14p〜6 np〜1(n〜= 7,8)和双激发4s〜24p〜45s〜1 6p〜1共振的泵浦探针光电子速度图成像

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Pump-probe photoelectron velocity-map imaging, using 27-eV high-harmonic excitation and 786-nmionization, is used to resolve overlapping autoionizing resonances in atomic krypton, obtaining two-photonphotoelectron angular distributions (PADs) for singly and doubly excited states. Two features in the photoelectronspectrum are assigned to singly excited 4s~1 4p~6 np~1 (n =7,8) configurations and four features provide informationabout double excitation configurations. The anisotropy parameters for the singly excited 7p configuration aremeasured to be β_2 = 1.61 ± 0.06 and β_4 = 1.54 ± 0.16 while the 8p configuration gives β_2 = 1.23 ± 0.19and β_4 =0.60 ± 0.15. These anisotropies most likely represent the sum of overlapping PADs from states ofsinglet and triplet spin multiplicities. Of the four bands corresponding to ionization of doubly excited states, twoare assigned to 4s~24p~45s~16p~1 configurations that are probed to different J-split ion states. The two remainingdoubly excited states are attributed to a previously observed, but unassigned, resonance in the vacuum-ultravioletphotoabsorption spectrum. The PADs from each of the double excitation states are also influenced by overlapfrom neighboring states that are not completely spectrally resolved. The anisotropies of the observed doubleexcitation states are reported, anticipating future theoretical and experimental work to separate the overlappingPADs into the state resolved PADs. The results can be used to test theories of excited state ionization.
机译:使用27 eV高谐波激发和786离子化的泵浦探针光电子速度图成像,用于解决原子k中重叠的自电离共振,获得单激发态和双激发态的双光子光电子角分布(PAD)。光电子光谱中的两个特征分配给单激发4s〜1 4p〜6 np〜1(n = 7,8)配置,四个特征提供有关双激发配置的信息。单激发7p构型的各向异性参数测得为β_2= 1.61±0.06和β_4= 1.54±0.16,而8p构型的各向异性参数为β_2= 1.23±0.19和β_4= 0.60±0.15。这些各向异性最有可能代表来自单重态和三重态自旋多重性的重叠PAD的总和。在对应于双激发态电离的四个频带中,有两个被分配给4s〜24p〜45s〜16p〜1构型,分别探测不同的J分裂离子态。剩下的两个双激发态归因于先前在真空-紫外光吸收光谱中观察到的但未分配的共振。来自每个双激发态的PAD也会受到来自相邻态的重叠的影响,这些重叠没有被完全光谱分辨。报告了观察到的双激发态的各向异性,从而预期了将来将重叠的PAD分离为状态分辨的PAD的理论和实验工作。该结果可用于测试激发态电离的理论。

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