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those that are diffracted by the regular array of lattice planes in a crystalline structure and therefore carry crystallographic information. A crystal will generate discrete diffracted beams whereas an amorphous material will produce diffuse rings. Imaging with Bragg diffracted electrons is called DF imaging as vacuum will show up dark. In the TEM mode one or several Bragg diffracted beams can be selected with the objective aperture, whereas in STEM mode, an annular solid-state detector averages over all Bragg diffracted electrons. This is called annular dark eld (ADF) imaging and is equivalent to conical dark eld imaging in TEM. Further away from the optical axis, where the intense Bragg diffracted electron signal fades, the Rutherford scattered electrons, those that have been scattered by the sample s nuclei, can be recorded. Figure 5.7.2 schematizes the location of Bragg diffracted and Rutherford scattered electrons around the optical axis. Rutherford scattered electrons carry atomic mass or Z-contrast, just as the backscattered electrons in the SEM (also Rutherford scattering) and since they also are recorded with an annular detector, but with a vb.net gs1 128 Packages matching GS1-128 - NuGet Gallery
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