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Figure 5
Sketch explaining the main idea of our approach: the higher the feature (2) on the surface, the quicker its growth occurs due to polymerization of incoming molecules. The distribution of the field intensity (1) near the carbon surface was calculated assuming an incidence of soft X-rays of 10 nm wavelength at 3° grazing angle. The z-axis is directed into the substrate.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 23| Part 1| January 2016| Pages 78-90
doi:10.1107/S160057751502202X
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