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2011 | OriginalPaper | Buchkapitel

2. Energy-Loss Instrumentation

verfasst von : R.F. Egerton

Erschienen in: Electron Energy-Loss Spectroscopy in the Electron Microscope

Verlag: Springer US

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Abstract

Complete characterization of a specimen in terms of its inelastic scattering would involve recording the scattered intensity J(x, y, z, θ x , θ y , E) as a function of position (coordinates x, y, z) within the specimen and as a function of scattering angle (components θ x and θ y ) and energy loss E. For an anisotropic crystalline specimen, the procedure would have to be repeated at different specimen orientations. Even if technically feasible, such measurements would involve storing a vast amount of information, so in practice the acquisition of energy-loss data is restricted to the following categories (see Fig. 2.1):

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Fußnoten
2
If TRANSPORT is used to calculate the matrix elements, a multiplying factor of 1000 is required on the right-hand side of Eq. (2.15) as a result of the units (x in cm, x′ in mrad, and δ in %) used in that program.
 
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Metadaten
Titel
Energy-Loss Instrumentation
verfasst von
R.F. Egerton
Copyright-Jahr
2011
Verlag
Springer US
DOI
https://doi.org/10.1007/978-1-4419-9583-4_2

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