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Oscillations, Waves, and Interactions - GWDG

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436 S. Lakämper <strong>and</strong> C. F. Schmidt<br />

interest. In contrast to conventional microscopy, the AFM reports the response of the<br />

imaged objects to the force exerted by the tip which can give more than just structural<br />

information about the sample. While generally rather slow compared to, e. g.,<br />

video microscopy, AFM provides nanometre or better resolution <strong>and</strong> therefore can<br />

resolve details of bio-macromolecules that are otherwise only accessible by electron<br />

microscopy or X-ray crystallography.<br />

The AFM furthermore allows one to measure forces with piconewton resolution.<br />

This capability can be used to mechanically probe single molecules, but also biopolymers,<br />

such as DNA or protein chains, <strong>and</strong> determine rigidity, rupture forces or unfolding<br />

forces. AFM-imaging of biomolecules is generally still a slow technique, requiring<br />

10 s or more of seconds per frame. We are especially interested in new developments<br />

aiming for imaging at video rates in order to capitalize on the capability of AFM to<br />

monitor structure, mechanics <strong>and</strong> dynamics at the same time in physiological conditions.<br />

AFM can also be combined with fluorescence microscopy which adds specific<br />

recognition.<br />

1.2 Fluorescence microscopy<br />

Light microscopy <strong>and</strong> especially fluorescence microscopy has experienced a renaissance<br />

with the advent of laser illumination <strong>and</strong> highly photo-stable chemical <strong>and</strong> biological<br />

fluorophores. We are especially focussing on the imaging of single molecules.<br />

The development of specific labelling strategies <strong>and</strong> of highly sensitive detection<br />

methods <strong>and</strong> cameras have made the real-time observation of single molecules – in<br />

vitro – or even in living organisms – in vivo – possible.<br />

To be able to detect single molecules, the background fluorescence needs to be<br />

sufficiently low. Two approaches are used in the lab: using total internal reflection<br />

of a laser-beam on the glass–water interface of the sample chamber, the (evanescent<br />

wave) illumination-depth within the sample is reduced to 100–200 nm. This<br />

drastically reduces the background fluorescence, as the typically tens of µm-thick<br />

samples are not completely illuminated. The other approach is to use wide-field illumination<br />

<strong>and</strong> strongly reduce the concentration of active fluorescent proteins. The<br />

latter approach allows better control over illumination intensities <strong>and</strong> the bleaching<br />

processes. Furthermore, we are currently developing multi-colour single molecule fluorescence<br />

setups to use Förster-Resonance Energy Transfer (FRET) between pairs<br />

of fluorophores. Since the energy transfer is strongly dependent on distance, it can<br />

be used to monitor domain <strong>and</strong>/or sub-unit interactions of proteins (molecular motors/chaperonins)<br />

on the nanometre scale.<br />

Diffraction-limited imaging of single fluorophores results in diffraction patterns<br />

of size ∼ λ/2 which limits the spatial resolution in densely labeled samples. An<br />

individual fluorophore can, however, be localized by fitting the diffraction pattern of<br />

a point source with accuracies better than 2 nm, which provides valuable information<br />

about the dynamics of molecular machines. The accuracy of position detection <strong>and</strong><br />

relative shifts can be combined with or complemented by the sub-nm resolution of<br />

optical trapping techniques.

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