Topography
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Topography imaging at the nanoscale is one of the main scopes of
AFM. Analysis of chemical composition and
structure of various blends, block-copolymers, fibres, crystallites
and single molecules is primarily based on
visualization of topography data. Different processes like crystallizing/melting,
wetting/dewetting, diffusion,
adsorption, self-assembly and chemical reactions can also be visualized
using topography scans.
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| Fig. 1 Height image showing the coexistence
of spherical and cylindrical micelles of PS-b-PI block-copolymers
in n=heptane.* Scan size 1.2 µm. |
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Basically, there are three different AFM modes used for topography
imaging, which are Non-contact mode, Contact mode and Tapping mode.
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Tapping mode
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Tapping mode is widespread for its ability of non-destructive high-resolution
imaging of soft and fragile samples in ambient conditions. The success
of the experiment depends not only on a correctly chosen probe but
to a large extent on optimal imaging routine. A minimal tip-sample
force, a properly adjusted feedback and an appropriate scanning
rate are a combination of important parameters for most precise
topographic imaging. The minimization of the tip-force in tapping
mode is achieved by choosing set-point amplitude (Asp)
as close as possible to the amplitude of free-oscillating probe
(A0).
Due to a number of instrumental imperfections (stability of laser,
variations in mechanical coupling between the probe and its holder,
thermal drift, etc) it is rather difficult to insure high stability
of the amplitude and to conduct imaging say at Asp =
0.99A0. Due to these imperfections one can observe a
slow change of the imaging contrast during scan. Thermal drift is
one of the important factors influencing imaging in amplitude modulation
modes, such as tapping mode. High quality factors of the probe places
time restrictions for feedback mechanism and imaging in tapping
mode should be conducted relatively slow with scanning rate not
much exceeding 1 Hz. These rates are recommended for imaging areas
below 1 µm X 1 µm, and the rates are smaller for scanning
larger areas.
In many cases, one can use moderately stiff cantilevers of the
DP14 series (~1 N/m) and General Purpose tips with radius ~10nm,
which provide good-quality images for a broad variety of samples.
The choice of the probe tip is determined by the resolution needed
in the experiment. When imaging conditions are optimized than sequential
images of the same area will be almost identical.
It might be also useful at the end of the studies of the particular
area to make a final scan on a large area that includes the location
where multiple scans were made. In some cases you might find that
imaging of the smaller area left a "window" seen in the
large scan. This will be a strong indication that tip-force should
be minimized further either by choosing smaller A0 (still
keeping Asp close to A0) or by taking softer
probes (DP18/GP or even softer DP09/GP).
Tapping mode in liquid requires cantilevers with a relatively low
resonant frequency. It is generally recommended to use uncoated
cantilevers in liquids or probes with overall chemically stable
Cr-Au coating having tip radius about 50 nm.
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Contact mode
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Contact mode is a high-speed AFM technique, which is mainly used
to image hard surfaces when the presence of lateral forces is not
expected to modify the morphological features. Conventional Contact
mode cantilever for using in air has a normal spring constant of
0.9 N/m and Aluminum coating on the backside. The choice of resolution
is limited to GP and LS tips.
Though the backside coating is stable in air and some fluids like water and ethanol, it dissolves readily in caustic alkali
solutions to give aluminum hydroxide. Uncoated probes or probes with overall chemically inert Cr-Au coating having
larger tip radius about 50 nm are recommended for using in aggressive liquid media.
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Noncontact mode
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In non-contact mode the tip-sample interaction is minimized. Ultrahigh
vacuum conditions are essential in this mode as small amplitudes
of oscillation and small tip-sample distance are used to enhance
the sensitivity to short-range tipsample forces. High spring constant
of 20..100 N/m is required to avoid tip sticking to surface at small
amplitudes. Cantilevers with higher resonant frequency are preferable
as they are faster and less noisy, use low-frequency probes only
if your system does not support probes with short lever arms.
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| * LaRue, I.; Adam, M.; Pitsikalis, M.; Hadjichristidis,
N.; Rubinstein, M.; Sheiko, S.S. "Reversible Morphological Transitions
of Polystyrene-b-Polyisoprene Micelles" Macromolecules 39, 309-314
(2006). |
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