Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Noncontact Atomic Force Microscopy - Yale School of Engineering ...
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Tu-1530<br />
The Effective Quality Factor in Dynamic <strong>Force</strong> Microscopes with<br />
Fabry-Perot Interferometer Detection<br />
Hendrik Hölscher 1 , Peter Milde 2 , Ulrich Zerweck 2 , Lukas M. Eng 2 , Regina H<strong>of</strong>fmann 3<br />
1 Institute for Microstructure Technology (IMT), Forschungszentrum Karlsruhe, Karlsruhe, Germany<br />
2 Institut für Angewandte Photophysik, Technische Universität Dresden, Germany<br />
3 Physikalisches Institut and DFG-Center for Functional Nanostructures, Universität Karlsruhe, Germany<br />
Recently, the self-oscillation <strong>of</strong> micr<strong>of</strong>abricated silicon resonators by photo-induced<br />
forces has become a focus <strong>of</strong> current research in order to reach the quantum ground state<br />
[1]. Having these results in mind, it is interesting to note that the experimental set-up<br />
used in these studies is similar in design to the standard instrumentation <strong>of</strong> lowtemperature<br />
ultra-high vacuum atomic force microscopes (LT-UHV-AFM) using<br />
interferometer detection [2,3].<br />
In order to quantify the relevance <strong>of</strong> photo-induced forces for NC-AFM<br />
experiments, we analyzed the oscillation behavior <strong>of</strong> a micr<strong>of</strong>abricated cantilever in a<br />
LT-UHV-AFM with a Fabry-Perot interferometer. We observed that photo-induced<br />
forces depend on the cantilever-fiber distance and that they lead to a pr<strong>of</strong>ound change <strong>of</strong><br />
the effective quality factor <strong>of</strong> the cantilever. Depending on the slope <strong>of</strong> the interference<br />
signal, the effective quality factor <strong>of</strong> the cantilever is increased or decreased. The overall<br />
effect increases with the laser power <strong>of</strong> the laser diode and decreases for higher<br />
temperatures. The Q-factor <strong>of</strong> the cantilever, however, is an essential parameter when the<br />
energy dissipation between tip and sample is measured with a dynamic force microscope.<br />
Hence, the effect addressed here has to be taken into account whenever the cantilever<br />
oscillation is measured with an interferometer at low temperatures.<br />
a) b) c)<br />
Figure 1: (a) Schematic set-up <strong>of</strong> the interferometer used for the detection <strong>of</strong> the cantilever<br />
vibration in dynamic force microscopy (b) The resulting interference intensity is periodic and has<br />
a positive or negative slope. (c) Depending on the slope and the temperature the resonance curves<br />
change dramatically due to a change <strong>of</strong> the effective Q-factor <strong>of</strong> the cantilever.<br />
[1] C. Höberger-Metzger and K. Karrai, Nature 432, 1002 (2004).<br />
[2] D. Rugar, H. J. Mamin, and P. Guethner, Appl. Phys. Lett. 55, 2588 (1989).<br />
[3] A. Moser et al., Meas. Sci. Technol. 4, 769 (1993).<br />
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