Fluorine Kα x‐ray fluorescence spectra of LuF 3  and NaF using synchrotron radiation | Zendy

Kaibuchi Kazuki | Zendy; Nagasono Mitsuru | Zendy; Liu Zhenlin | Zendy; Koja Yusuke | Zendy; Fukushima Akiko | Zendy; Shin Shik | Zendy; Takahashi Hideyuki | Zendy; Kawai Jun | Zendy

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Fluorine Kα x‐ray fluorescence spectra of LuF 3 and NaF using synchrotron radiation

Author(s) -

Kaibuchi Kazuki,

Nagasono Mitsuru,

Liu Zhenlin,

Koja Yusuke,

Fukushima Akiko,

Shin Shik,

Takahashi Hideyuki,

Kawai Jun

Publication year - 2005

Publication title -

surface and interface analysis

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.52

H-Index - 90

eISSN - 1096-9918

pISSN - 0142-2421

DOI - 10.1002/sia.1962

Subject(s) - synchrotron radiation , fluorescence , excited state , spectral line , synchrotron , radiation , emission spectrum , atomic physics , x ray fluorescence , line (geometry) , x ray , chemistry , satellite , intensity (physics) , analytical chemistry (journal) , physics , optics , geometry , mathematics , chromatography , astronomy

The F Kα x‐ray fluorescence spectrum of LuF 3 is excited by monochromated synchrotron radiation and a satellite peak is observed at the higher energy side of the F Kα 1, 2 lines. The intensity of this peak depends on the incident x‐ray energy; the presence of the threshold energy to excite the satellite proves that the satellite is assigned to Kα 3, 4 due to the transition 1s −1 2p −1 → 2p −2 . The K α3, 4 /K α1, 2 intensity ratio for LuF 3 is 0.20, which is significantly weaker than that for NaF (0.46). It is observed that the Kα 1, 2 line width of LuF 3 is significantly broader than that for NaF. Copyright © 2005 John Wiley & Sons, Ltd.

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