Beilstein J. Nanotechnol.2011,2, 252–260, doi:10.3762/bjnano.2.29
measured contact potential difference even under ultra-highvacuum conditions, and we demonstrate a good agreement between our model and KPFM measurements in ultra-highvacuum of NaCl monolayers grown on Cu(111). The effect of the oscillating cantilever shape on the KPFM resolution and sensitivity has been
cantilever in general, and in high resolution ultra-highvacuum (UHV) KPFM measurements in particular, has not been reported. In this work we use the boundary element method (BEM) [7] to calculate the point spread function (PSF) of the measuring probe: Tip and cantilever. The probe PSF analysis shows that
showed that at smaller probe sample distances the homogenous force contribution of the tip apex is higher. At a probe–sample distance of 1.2 nm (a typical distance in ultra-highvacuum measurements) the tip apex contributes 83% to the homogenous force, the cone lower segment contributes 7.3%, and the
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Figure 1:
(a) Geometrical model of a tip, with cone length l, half-aperture angle θ0, spherical apex radius R...
Beilstein J. Nanotechnol.2011,2, 85–98, doi:10.3762/bjnano.2.10
humidity), we have investigated how the nanomanipulation process is affected in ultrahighvacuum (UHV) environment. The topography image in Figure 7 shows the gold particles on a silicon substrate after the sample was transferred into UHV without any further treatment, which could have changed the
deposited onto a silicon wafer. (a) Ordered organization as described in the Experimental section, (b) random distribution. Frame sizes: 3 µm and 1 µm, respectively.
As-synthesized Au particles on silicon in ultra-highvacuum. Frame size: 3 µm.
AFM image of nanopatterned surface exhibiting Si pits: Frame
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Figure 1:
Evolution of the logarithm of the dissipated power normalized by the radius (R) as a function of (a...