Abstract

The phase shift induced by thin amorphous carbon films with thicknesses between 1 and 16 nm was measured by electron holography in a transmission electron microscope. Large phase shifts Δ φ are observed as the thickness of the amorphous C films decreases which cannot be described by the well-known equation Δ φ = C E V 0 t ( V 0: mean inner Coulomb potential of the material, t: sample thickness). Data plotted in a Δ φ vs. t diagram can be well-fitted by a modified equation Δ φ = C E V 0 t + φ add . The mean inner Coulomb potential of the amorphous carbon with a density of 1.75 g/cm 3 was determined to be 9.09 V which is consistent with previous experimental data for amorphous carbon with a higher density. The thickness-independent phase offset φ add of 0.497 rad is large for amorphous carbon under the given experimental conditions. We suggest that a surface-related electrostatic potential is responsible for the thickness-independent contribution φ add .

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