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The nanopore shrinking process can be stopped by blocking the electron beam.
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The electron beam causes the frozen sample block to warp, motion-blurring a traditional camera's images.
This technique involves the sample serial sectioning with the ion beam, thus generating new block faces, which are then imaged at high resolution with the electron beam.
To further improve the vacuum, the substrate is blocked from flux via a shutter and chromium (Cr) is deposited onto the chamber walls using the electron beam source.
A 30-nm HfO2 film deposited by the electron beam (E-beam) evaporation system with a base pressure of 3.6 × 10−6 Torr served as the blocking layer.
The full line indicates the electron beam divergence angle.
b, Bragg peak intensity changes probed by the electron beam.
The first grid next to the cathode controls the number of electrons in the electron beam and focuses the beam.
After the electron beam has exited the helix, the electrons are decelerated by a multistage collector.
Because electrons cannot travel very far in air, the electron beam and the sample must be kept in a vacuum.
In electron storage rings, stochastic emission of synchrotron radiation photons heats up the electron beam.
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