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@INPROCEEDINGS{Zheng:827183,
author = {Zheng, Fengshan and Migunov, Vadim and Ramsperger, Urs and
Pescia, Danilo and Dunin-Borkowski, Rafal},
title = {{Q}uantitative measurement of the charge distribution along
a tungsten nanotip using transmission electron holography},
address = {Weinheim, Germany},
publisher = {Wiley-VCH Verlag GmbH $\&$ Co. KGaA},
reportid = {FZJ-2017-01381},
pages = {737 - 738},
year = {2016},
abstract = {Off-axis electron holography can be used to measure the
electron-optical phase shift associated with a charge
density distribution in the transmission electron microscope
(TEM). The charge density can then be recovered either by
integrating the Laplacian of the reconstructed phase1 or,
equivalently, by applying a loop integral2. Whichever
approach is used, the perturbed reference wave3 does not
affect the measurement of the projected charge density
inside the specimen so long as it does not itself contain
any charges. Here, we study a W nanotip, in which the charge
density distribution is of interest for applications in
field emission and atom probe tomography. We assess
artefacts and noise in the measurements.Figure 1(a) shows an
off-axis electron hologram of a W nanotip recorded at 300 kV
using an FEI Titan 60-300 TEM. The interference fringe
spacing is 0.318 nm, the nominal magnification is 140 000
and the voltage applied to the electrostatic biprism is 90
V. The apex of the nanotip has a diameter of approximately 5
nm and is covered with a layer of tungsten oxide. A voltage
of 50 V was applied between the nanotip and a flat electrode
positioned approximately 3 µm away from it. In order to
remove the contribution to the phase shift from the mean
inner potential, two holograms with and without a voltage
applied to the nanotip were recorded. The difference between
the two phase images was then evaluated after sub-pixel
alignment. Figures 1(b) and (c) show the resulting unwrapped
phase before and after adding phase contours of spacing
2π/3 radians. Figure 1(d) shows the charge distribution
calculated by applying a Laplacian operator to a
median-filtered version of the phase image. Figure 1(e)
shows cumulative charge profiles along the nanotip
determined both using a loop integral and by applying a
Laplacian operator to either an unwrapped phase image or the
original complex image wave. The integration region is
marked by a green dashed rectangle in Fig. 1 (b). The
measured charge profile is consistent between the three
approaches. Figure 1(f) shows an evaluation of noise in the
measurement obtained by performing a similar integration in
a region of vacuum indicated by the red dashed rectangle in
Fig. 1(b). Results such as those shown in Figs. 1(d) and (e)
can be used to infer the electric field and electrostatic
potential around the tip. Future work will involve comparing
the present approaches with using a model-based technique
for determining the charge density from a recorded phase
image.},
month = {Aug},
date = {2016-08-28},
organization = {16th European Microscopy Congress (EMC
2016), Lyon (France), 28 Aug 2016 - 2
Sep 2016},
cin = {PGI-5 / ER-C-1},
cid = {I:(DE-Juel1)PGI-5-20110106 / I:(DE-Juel1)ER-C-1-20170209},
pnm = {143 - Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)8},
doi = {10.1002/9783527808465.EMC2016.6252},
url = {https://juser.fz-juelich.de/record/827183},
}