Argon KLL Auger spectrum: Initial states, core-hole lifetimes, shake, and knock-down processes

被引:16
作者
Puettner, Ralph [1 ]
Holzhey, Philippe [1 ,11 ]
Hrast, Mateja [2 ]
Zitnik, Matjaz [2 ,3 ]
Goldsztejn, Gildas [4 ,5 ]
Marchenko, Tatiana [4 ,6 ]
Guillemin, Renaud [4 ,6 ]
Journel, Loic [4 ,6 ]
Koulentianos, Dimitris [4 ,7 ,12 ]
Travnikova, Oksana [4 ,6 ]
Zmerli, Moustafa [4 ]
Ceolin, Denis [6 ]
Azuma, Yoshiro [8 ]
Kosugi, Satoshi [8 ]
Lago, Alexsandre F. [9 ]
Piancastelli, Maria Novella [4 ,10 ]
Simon, Marc [4 ,6 ]
机构
[1] Free Univ Berlin, Fachbereich Phys, D-14195 Berlin, Germany
[2] J Stefan Inst, Jamova 39, Ljubljana 1000, Slovenia
[3] Univ Ljubljana, Fac Math & Phys, Jadranska 19, Ljubljana 1000, Slovenia
[4] Sorbonne Univ, CNRS, Lab Chim Phys Matiere & Rayonnement, F-75005 Paris 05, France
[5] Univ Paris Saclay, CNRS, Inst Sci Mol Orsay, F-91405 Orsay, France
[6] Synchrotron SOLEIL, F-91192 Gif Sur Yvette, France
[7] Univ Gothenburg, Dept Phys, Origovagen 6B, S-41296 Gothenburg, Sweden
[8] Sophia Univ, Dept Mat & Life Sci, Tokyo 1028554, Japan
[9] Univ Fed ABC, Ctr Ciencias Nat & Humanas, BR-09210580 Santo Andre, SP, Brazil
[10] Uppsala Univ, Dept Phys & Astron, S-75120 Uppsala, Sweden
[11] Univ Oxford, Dept Phys, Clarendon Lab, Oxford OX1 3PU, England
[12] Argonne Natl Lab, Chem Sci & Engn Div, 9700 South Cass Ave, Lemont, IL 60439 USA
基金
欧盟地平线“2020”;
关键词
Photons - Augers - Orbits - Auger electron spectroscopy - Photoelectron spectroscopy - Photoelectrons;
D O I
10.1103/PhysRevA.102.052832
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
State-of-the-art argon KLL Auger spectra measured using photon energies of h nu = 3216 and 3400 eV are presented along with an Ar [1s] photoelectron spectrum (square brackets indicate holes in the respective orbital). The two different photon energies used for measuring the Auger spectra allow distinguishing between the shake transitions during the Auger decay and the Auger transitions of the photoelectron satellites. A complete assignment of satellite transitions is provided, partially based on configuration-interaction calculations. In addition, Ar [1s3(s, p)]n'l' -> [2p(2)(1D(2))] transitions are observed, which can be explained by knock-down transitions leading to a direct exchange of angular momentum between the excited electron and the Auger electron. The lifetime broadenings of the Ar [2s] single-core-hole state and the [2s(2)] and [2s2p] double-core-hole states are also determined, confirming previously observed trends for double-core-hole states.
引用
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页数:14
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