Thesis-PDF - IAP/TU Wien
Thesis-PDF - IAP/TU Wien
Thesis-PDF - IAP/TU Wien
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Figure 3.6: Highly ordered and freshly cleaved pyrolytic graphite at atomic<br />
resolution imaged with an AFM in UHV. Image adapted from [8].<br />
characteristic for a collection of atoms like electrostatic, magnetic, tribological,<br />
and viscoelastic properties.<br />
A selection of the most widely used techniques is given beneath.<br />
3.3.1 Single Atom and Molecule Information<br />
- Position of single atoms and single molecules (e.g. pyrolytic graphite in Fig.<br />
3.6)<br />
- Chemical identification of individual surface atoms. The onset of chemical<br />
bonding between the approaching tip and surface atoms gives rise to shortrange<br />
forces that depend sensitively on the chemical identity of the atoms<br />
involved. These can be measured by sensitive AFM. (Tin (Sn), Silicon (Si),<br />
Lead (Pb) as detected by AFM can be seen in Fig. 3.7, [47])<br />
- Molecular recognition studies using AFM open the possibility to detect<br />
specific ligand–receptor interaction forces and to observe molecular recognition<br />
of a single ligand–receptor pair. The approach is to bind either ligand<br />
or receptor to the AFM tip when its counterpart should be found on the<br />
investigated surface. In a force–distance cycle (as graphed by a force curve,<br />
see below), the tip is approached towards the surface and, if the counterpart<br />
is present, a receptor–ligand complex is formed because of the specific ligand<br />
receptor recognition. Upon retraction an increased force (unbinding force)<br />
must be exerted in order to break the ligand–receptor connection (e.g. antibody<br />
binding and recognition in [48]). Such experiments allow for estimation<br />
of affinity, rate constants, energies ([49]) and structural data of the binding<br />
pocket ([48], [50], [51], [52], [53], [54]). There have also been attempts to<br />
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