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Non-topographic current contrast in scanning field emission microscopy
Author(s) -
Gabriele Bertolini,
O. Gürlü,
Robin Pröbsting,
D. Westholm,
Jiapeng Wei,
U. Ramsperger,
D.A. Zanin,
H. Cabrera,
D. Pescia,
J. P. Xanthakis,
M. Schnedler,
Rafal E. DuninBorkowski
Publication year - 2021
Publication title -
royal society open science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.84
H-Index - 51
ISSN - 2054-5703
DOI - 10.1098/rsos.210511
Subject(s) - field electron emission , quantum tunnelling , monatomic ion , field (mathematics) , optics , current (fluid) , contrast (vision) , materials science , scanning tunneling microscope , microscopy , physics , electron , optoelectronics , nanotechnology , mathematics , quantum mechanics , pure mathematics , thermodynamics
In scanning field emission microscopy (SFEM), a tip (the source) is approached to few (or a few tens of) nanometres distance from a surface (the collector) and biased to field-emit electrons. In a previous study (Zanin et al. 2016 Proc. R. Soc. A 472 , 20160475. ( doi:10.1098/rspa.2016.0475 )), the field-emitted current was found to change by approximately 1% at a monatomic surface step (approx. 200 pm thick). Here we prepare surface domains of adjacent different materials that, in some instances, have a topographic contrast smaller than 15 pm. Nevertheless, we observe a contrast in the field-emitted current as high as 10%. This non-topographic collector material dependence is a yet unexplored degree of freedom calling for a new understanding of the quantum mechanical tunnelling barrier at the source site that takes into account the properties of the material at the collector site.

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