Fourier deconvolution of electron energy-loss spectra

Electron energy-loss spectroscopy (e. e. l. s.) performed with an electron microscope can be used to obtain plasmon spectra, near-edge fine structure and extended electron energy-loss fine structure (ex. e. l. f. s.), as well as to do chemical analysis on truly microscopic samples. However, the very strength of the electron–electron interaction gives rise to significant and sometimes predominant plural scattering effects. To obtain consistent and reliable estimates of the single scattering distributions these effects must be accounted for. In this paper, two Fourier-transform deconvolution methods of removing plural scattering from electron energy-loss spectra and their implementation on a microcomputer, are discussed. Their relative advantages and limitations are considered together with examples of artefacts that may arise in both plasmon and core-loss spectra. As a result of deconvolution the sensitivity and accuracy of core-elemental analysis is enhanced but, more importantly, it is possible to obtain reproducible near-edge structure and plasmon spectra from relatively thick samples that would otherwise not be suitable for investigation by means of e. e. l. s.

2000 ◽  
Vol 6 (S2) ◽  
pp. 186-187
Author(s):  
D. A. Pankhurst ◽  
G. A. Botton ◽  
C. J. Humphreys

It has been demonstrated that electron energy loss spectrometry (EELS) can be used to probe the electronic structure of materials on the near-atomic scale. The electron energy loss near edge structure (ELNES) observed after the onset of a core edge reflects a weighted local density of final states to which core electrons are excited by fast incident electrons. Lately ‘atomic resolution EELS’ and ‘column-by-column spectroscopy’ have become familiar themes amongst the EELS community. The next generation of STEMs, equipped with spherical aberration (Cs) correctors and electron beam monochromators, will have sufficient spatial and energy resolution, along with the superior signal to noise required, to detect small changes in the ELNES from atomic column to atomic column.Core loss ELNES provides information about unoccupied states, but the structure observed in spectra is sensitive to changes in the underlying occupied states, and thus to the bonding in the material.


1986 ◽  
Vol 33 (1) ◽  
pp. 22-24 ◽  
Author(s):  
Th. Lindner ◽  
H. Sauer ◽  
W. Engel ◽  
K. Kambe

1993 ◽  
Vol 218 (1-2) ◽  
pp. 301-308 ◽  
Author(s):  
A. Balzarotti ◽  
F. Arciprete ◽  
S. Colonna ◽  
M. Diociaiuti ◽  
F. Patella ◽  
...  

Author(s):  
H. Sauer ◽  
R. Brydson ◽  
W. Engel ◽  
P.N. Rowley

The electron energy-loss near-edge structure (ELNES) associated with a core-loss edge measured using electron energy-loss spectroscopy (EELS) provides, in favourable cases, a “fingerprint” corresponding to the specific nearest-neighbour coordination of the excited atom.Boron atoms in boron-oxygen compounds occur in both trigonal (BO3) and tetrahedral (BO4) coordinations. The B K-ELNES of BO3 and BO4 units (Figs, le and 2b) are remarkably different and arise from the differing local symmetries which determine the final state molecular orbitals. The BK-ELNES of BO3 units exhibit a sharp π∗ peak at ca. 194 eV followed by a broader σ∗ peak some 9-10 eV higher in energy, which may possess a low energy shoulder. BO4 B K-ELNES show no π∗ peak and display solely a σ∗ peak at ca. 199 eV together with a high energy shoulder. Both these spectra may be modelled using multiple scattering calculations.The mineral howlite contains both BO3 and BO4 units and is sensitive to electron-beaminduced damage.


2007 ◽  
Vol 13 (S02) ◽  
Author(s):  
C Witte ◽  
NJ Zaluzec ◽  
SD Findlay ◽  
LJ Allen

2000 ◽  
Vol 61 (3) ◽  
pp. 2180-2187 ◽  
Author(s):  
Teruyasu Mizoguchi ◽  
Isao Tanaka ◽  
Masato Yoshiya ◽  
Fumiyasu Oba ◽  
Kazuyoshi Ogasawara ◽  
...  

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