Issue |
Eur. Phys. J. Appl. Phys.
Volume 70, Number 2, May 2015
|
|
---|---|---|
Article Number | 20701 | |
Number of page(s) | 15 | |
Section | Imaging, Microscopy and Spectroscopy | |
DOI | https://doi.org/10.1051/epjap/2015150075 | |
Published online | 21 May 2015 |
https://doi.org/10.1051/epjap/2015150075
Photoelectron spectroscopy of transition metal oxide interfaces
Diamond Light Source Ltd., Harwell Science and Innovation Campus, Didcot OX11 0DE, UK
a e-mail: jorg.zegenhagen@diamond.ac.uk
Received:
5
February
2015
Revised:
23
March
2015
Accepted:
14
April
2015
Published online:
21
May
2015
In the present paper we review applications of the photoelectron spectroscopy (PES) technique to the investigation of transition metal oxide (TMO) interfaces. We summarize very briefly some of the principle, specific characteristics of TMOs. Because of the buried nature of the interfaces, the photoelectrons must penetrate certain thicknesses of material, which is easier with higher kinetic energies in the keV range. Thus, we also briefly summarize some of the hallmarks of hard X-ray photoelectron spectroscopy (HAXPES), before presenting four explicit samples of the analysis of TMO interfaces: The LaAlO3/SrTiO3 (0 0 1) interface, which had attracted attention because of the discovery of a sheet of high mobility electrons below the thin layer of LaAlO3; superlattices of the two insulators CaCuO2 and SrTiO3, which can be prepared to become superconducting at about 40 K; epitaxial films of the 90 K superconductor GdBa2Cu3O7−δ on NdGaO3; and finally the analysis of the nucleation of the 90 K superconductor YBa2Cu3O7−δ on SrTiO3 (0 0 1). The latter two cases of the investigation of the superconducting films are examples of photoelectron spectroscopy by X-ray standing wave (XSW) excitation. Because of this, the bare essential features of the XSW technique are also briefly reviewed.
© EDP Sciences, 2014
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