2010
DOI: 10.1016/j.micron.2010.05.014
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Determination of the linear attenuation range of electron transmission through film specimens

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Cited by 13 publications
(5 citation statements)
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“…This difference between the two tomography results indicates the effect of inelastically scattered electrons with increasing sample proportion in the 1.0‐µm‐thick section. Similarly, increasing the electron beam path length at higher tilt angles also leads to image degradation due to multiple scattering (Wang et al ., 2010a, b, c). In addition to these factors, the depth of focus must be considered when observing thick sections at magnifications above 10 000× (Hayashida & Malac, 2016).…”
Section: Discussionmentioning
confidence: 99%
“…This difference between the two tomography results indicates the effect of inelastically scattered electrons with increasing sample proportion in the 1.0‐µm‐thick section. Similarly, increasing the electron beam path length at higher tilt angles also leads to image degradation due to multiple scattering (Wang et al ., 2010a, b, c). In addition to these factors, the depth of focus must be considered when observing thick sections at magnifications above 10 000× (Hayashida & Malac, 2016).…”
Section: Discussionmentioning
confidence: 99%
“…Contrast is caused by differences in diffraction, phase, thickness and mass. By blocking diffracted beams with an aperture in the back focal plane a bright field (BF) image is obtained and this increases the diffraction contrast, because diffracted areas then appear darker [68]. A BF micrograph is shown in Figure 4.3.…”
Section: Transmission Electron Microscopymentioning
confidence: 99%
“…One of the major challenges in the application of EELS in transmission in solid-state physics and material science is the preparation of the samples. The mean free path of electrons in solids is limited due to a number of interactions, predominantly plasmon excitations [7,[42][43][44][45].…”
Section: Sample Preparationmentioning
confidence: 99%