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This title appears in the Scientific Report : 2009 

StripeSTEM, a technique for the isochronous acquisition of high angle annular dark-field images and monolayer resolved electron energy loss spectra

StripeSTEM, a technique for the isochronous acquisition of high angle annular dark-field images and monolayer resolved electron energy loss spectra

A technique capable of producing monolayer resolved electron energy loss (EEL) spectroscopy data along one direction in crystal structures is introduced. Unambiguous assignment of EEL spectra to atomic planes is possible via the execution of high angle annular dark-field (HAADF) imaging and EEL spec...

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Personal Name(s): Heidelmann, M.
Barthel, J. / Houben, L.
Contributing Institute: Mikrostrukturforschung; IFF-8
Published in: Ultramicroscopy, 109 (2009) S. 1447 - 1452
Imprint: Amsterdam Elsevier Science 2009
Physical Description: 1447 - 1452
DOI: 10.1016/j.ultramic.2009.07.007
PubMed ID: 19665304
Document Type: Journal Article
Research Program: Grundlagen für zukünftige Informationstechnologien
Erneuerbare Energien
Series Title: Ultramicroscopy 109
Subject (ZB):
J
STEM
EELS
Interfaces
Publikationsportal JuSER
Please use the identifier: http://dx.doi.org/10.1016/j.ultramic.2009.07.007 in citations.

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A technique capable of producing monolayer resolved electron energy loss (EEL) spectroscopy data along one direction in crystal structures is introduced. Unambiguous assignment of EEL spectra to atomic planes is possible via the execution of high angle annular dark-field (HAADF) imaging and EEL spectrum acquisition in parallel. The recording of instrumental instabilities in the HAADF image during the measurement enables a proper quantification by virtue of post-acquisition correction. Compared to the conventional line profile technique a dose reduction by several orders of magnitude can be achieved. The technique is applied to bulk SrTiO(3) and ZnO:In(2)O(3) in order to explore its capabilities and limits. Monolayer resolution was achieved for the Ti-L(23) and In-M(45) core-losses. Multislice calculations were carried out for the purpose of assessing the residual delocalisation of the inelastic signal. Fundamental limits to the resolution are imposed by dynamical dispersion of the electron wave in the crystal combined with the extension of the inelastic potential. In the present case, owing to the requirement of a high beam current, the geometrical probe size cannot be neglected when compared to the width of an inelastic scattering potential.

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