| Phase Imaging mode |
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| Semicontact | |
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Usage of Scanning Force Microscopy with oscillating cantilever was firstly anticipated by Binnig [1]. Earlier experimental realizations of scanning with oscillated cantilever was realized in works [2,3].
It was demonstrated influence of the force gradients on the cantilever
frequency shift and possibility of non-contact scanning sample surface.
It must be noted also that Durig studied frequency shift of oscillating
cantilever under influence of STM tip [4].
In [2] was demonstrated also possibility of materials sensing under abrupt decreasing of cantilever oscillation amplitude. Possibility of scanning sample surface not only in attractive but also in repulsive forces was demonstrated in [4]. Relatively small shift of oscillating frequency with sensing repulsive forces means that contact of cantilever tip with sample surface under oscillation is not constant. Only during small part of oscillating period the tip "feels" contact repulsive force. Especially it concerns to oscillations with relatively high amplitudes. Scanning sample surface with cantilever oscillated in this manner is not non-contact, but intermittent contact.
When probe tip under vibrating touches the sample
surface it experiences not only repulsive but also adhesive, capillary
and some other forces. So interaction of the tip with sample surface
results not only in frequency but in the phase shift as well. If the
sample surface is not homogeneous the same must be phase shift under
scanning sample surface. Distribution of the phase shift under scanning
over the sample surface reflects distribution of the sample material
characteristics. Such mode of operation when phase shift under scanning
is registered (Phase Contrast Imaging mode) is very useful for
materials investigation.
References
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