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Beilstein J. Nanotechnol. 2011, 2, 394–404, doi:10.3762/bjnano.2.45
Figure 1: Analysis of atomic contrast for different TEM conditions at 80 kV obtained using a code of E. Kirkl...
Figure 2: WIEN2k starting potential (red) compared to Doyle–Turner (black) and Kirkland (green) potentials. T...
Figure 3: Projected potential near the core at very high resolution (green line). The blue boxes indicate the...
Figure 4: Relaxed structure model of boron and oxygen substitution in graphene. Bond lengths are given in Å.
Figure 5: Analysis of the projected electron charge density of the boron (top) and oxygen substitution in gra...
Figure 6: Analysis of the projected potential of the boron (top) and oxygen substitution in graphene (bottom ...
Figure 7: TEM image simulation of boron substitution in graphene for an electron energy of 80 keV. The upper ...
Figure 8: TEM image simulation of oxygen substitution in graphene for the same conditions used in Figure 7.
Figure 9: Difference between the 3d electron charge density (center column) and the 3d electrostatic potentia...
Figure 10: TEM image simulation of an oxygen adatom on graphene for 80 kV. The first row is for Scherzer condi...