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A stable LaB(6) nanoneedle field-emission point electron source

A material with a low work function exhibiting field-emission of electrons has long been sought as an ideal point electron source to generate a coherent electron beam with high brightness, long service life, low energy spread, and especially stable emission current. The quality and performance of th...

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Detalles Bibliográficos
Autores principales: Tang, Shuai, Tang, Jie, Uzuhashi, Jun, Ohkubo, Tadakatsu, Hayami, Wataru, Yuan, Jinshi, Takeguchi, Masaki, Mitome, Masanori, Qin, Lu-Chang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: RSC 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9419243/
https://www.ncbi.nlm.nih.gov/pubmed/36134182
http://dx.doi.org/10.1039/d1na00167a
Descripción
Sumario:A material with a low work function exhibiting field-emission of electrons has long been sought as an ideal point electron source to generate a coherent electron beam with high brightness, long service life, low energy spread, and especially stable emission current. The quality and performance of the electron source are now becoming limiting factors for further improving the spatial resolution and analytical capabilities of the electron microscope. While tungsten (W) is still the only material of choice as a practically usable field emission filament since it was identified more than six decades ago, its electron optical performance remains unsatisfactory, especially the poor emission stability (>5% per hour), rapid current decay (20% in 10 hours), and relatively large energy spread (0.4 eV), even in an extremely high vacuum (10(−9) Pa). Herein, we report a LaB(6) nanoneedle structure having a sharpened tip apex with a radius of curvature of about 10 nm that is fabricated and finished using a focused ion beam (FIB) and show that it can produce a field emission electron beam meeting the application criteria with a high reduced brightness (10(10) A m(−2) sr(−1) V(−1)), small energy spread (0.2 eV), and especially high emission stability (<1% fluctuation in 16 hours without decay). It can now be used practically as a next-generation field-emission point electron source.