Octahedral conversion of a-SiO2 host matrix by pulsed ion implantation

The results of measurements of X‐ray photoelectron spectra (XPS) of a‐SiO2 host material after pulsed implantation with [Mn+] and [Co+, Mn+] ions as well as DFT‐calculations are presented. The low‐energy shift is found in XPS Si 2p and O 1s core‐levels of single [Mn+] and dual [Co+, Mn+] pulsed ion‐...

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Published inphysica status solidi (b) Vol. 252; no. 10; pp. 2185 - 2190
Main Authors Zatsepin, D. A., Zatsepin, A. F., Boukhvalov, D. W., Kurmaev, E. Z., Gavrilov, N. V., Skorikov, N. A., von Czarnowski, A., Fitting, H.-J.
Format Journal Article
LanguageEnglish
Published Blackwell Publishing Ltd 01.10.2015
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Summary:The results of measurements of X‐ray photoelectron spectra (XPS) of a‐SiO2 host material after pulsed implantation with [Mn+] and [Co+, Mn+] ions as well as DFT‐calculations are presented. The low‐energy shift is found in XPS Si 2p and O 1s core‐levels of single [Mn+] and dual [Co+, Mn+] pulsed ion‐implanted a‐SiO2 (E = 30 keV, D = 2×1017 cm−2) with respect to those of untreated a‐SiO2. Similar changes are found in XPS Si 2p and O 1s of stishovite compared to those of quartz. This means that the pulsed ion implantation induces the local high pressure effect that leads to the appearance of SiO6‐structural units in a‐SiO2 host, forming “stishovite‐like” local atomic structure. This process can be described within an electronic bonding transition from the fourfold “quartz‐like” to sixfold “stishovite‐like” high‐pressure phase in the SiO2 host matrix. It is found that such octahedral conversion depends on the fluence and starts with doses higher than D = 3×1016 cm−2.
Bibliography:Russian Science Foundation - No. 14-22-00004
ArticleID:PSSB201552103
istex:67578573C33843AF34A2A85091B49863150E5333
ark:/67375/WNG-87HQTTL8-B
ISSN:0370-1972
1521-3951
DOI:10.1002/pssb.201552103