1990
DOI: 10.1016/0168-583x(90)90125-e
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The influence of crystal thickness on scattering and radiation of high-energy electrons in oriented crystals

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Cited by 15 publications
(16 citation statements)
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“…Further, under such finely-controlled conditions, no direct comparisons have been made to conventional lowdose methods for precisely the same dose rate and the same total dose. 15 Here, we report our observations of a repeatable reduction in damage when using pulsed electron packets generated via fs laser excitation of a photocathode in a modified TEM as compared to a conventional thermionic beam for precisely the same dose rate and accumulated dose. By using fs laser excitation to precisely control the electron-emission process, we confine the probability of emission to a temporal range of 300 fs (full-width at half-maximum, FWHM) 20 for extremely regular peak-to-peak emission times.…”
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confidence: 89%
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“…Further, under such finely-controlled conditions, no direct comparisons have been made to conventional lowdose methods for precisely the same dose rate and the same total dose. 15 Here, we report our observations of a repeatable reduction in damage when using pulsed electron packets generated via fs laser excitation of a photocathode in a modified TEM as compared to a conventional thermionic beam for precisely the same dose rate and accumulated dose. By using fs laser excitation to precisely control the electron-emission process, we confine the probability of emission to a temporal range of 300 fs (full-width at half-maximum, FWHM) 20 for extremely regular peak-to-peak emission times.…”
mentioning
confidence: 89%
“…Relative arrival times of 5,20, and 100 µs were tested for electron packets comprised of, on average, 1, 5, and 20 electrons. In general, damage increased with decreasing time 15 between electrons and with increasing electron number. Further, we find that improvements relative to conventional methods vanish once a threshold number of electrons per packet is reached.…”
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confidence: 90%
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