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Our results herald exciting prospects for microscopic material studies, enables electron lithography with fixed sample and beam and high resolution electronic chip inspection by structured electron illumination.
Fig. 2 Time-dependent resolution during prolonged electron illumination.
Hence, the observed dehydrogenation is solely induced by the electron illumination.
The second is that the NW bends and shrinks via electron illumination (Fig. 3b).
In turn, such electron illumination conditions are advantageous in terms of minimizing electron beam-induced alterations of the chemical reactions under examination.
The fact that the resolution degradation occurred gradually over tens of seconds (Fig. 2a) indicates that it is related to a dynamic response of the sample under the electron illumination.
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Monazite anhydrite interphase boundaries and (1 2 0) anhydrite twin boundaries were mobile at room temperature under electron beam illumination.
We have found that these space-charge interactions lead to significant broadening and displacement of the Bragg spots at currently realizable electron beam illumination conditions.
Yields of 140 250 μmol O2 h−1 and 1 7 μmol H2 h−1 were obtained and were found to depend on the physical properties and content of WO3, the concentration of the electron scavenger, illumination period and wavelength, and the radiation geometry.
Here we show an example of metallic particle coalescence induced merely by parallel electron beam illumination in TEM.
Electrostatic charging can be generated by various methods (laser, ion, or electron beam illumination, diverse electrodes, etc).. Charged patterns of sub-micrometer dimensions can be created using nanometer-sized probes, such as those employed in atomic force microscopy (AFM) [4, 5].
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