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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Temperature-dependent growth <strong>of</strong> C60 on CaF2(111)<br />
Felix Loske, Philipp Maaß, Jens Schütte, and Angelika Kühnle<br />
Department <strong>of</strong> Physics, Universität Osnarück, Barbarastraße 7, 49076 Osnabrück ,Germany<br />
E-Mail: floske@uos.de<br />
P.II-05<br />
Non-contact atomic force microscopy was employed to study the system <strong>of</strong> C60<br />
molecules on the CaF2(111) surface in-situ at various temperatures. The molecules were<br />
observed to be very mobile on the surface at room temperature (RT), as they nucleate at<br />
step edges and form large islands on the terraces. Both, regular triangular islands as well<br />
as branched structures were observed to coexist (Fig. 1b and 1c). The branched structures<br />
were seen to change shape during measuring. S. Burke et al. have previously reported<br />
about such branched structures on alkali halides [1].<br />
The compact islands <strong>of</strong> C60 on CaF2 are at least two layer high, and at higher coverages<br />
C60 molecules grow in a dendritic manner onto the these compact C60 islands (Fig. 1d). In<br />
contrast, at low temperatures (LT) hexagonal islands are predominant, which are initially<br />
only one layer high. Here, already the second layer is growing in a dendritic manner (Fig.<br />
1a).<br />
These temperature-dependent measurements allow to gain insight into the molecular<br />
dynamics <strong>of</strong> this system and to specify the diffusion barrier. Microscopic growth models<br />
are shortly addressed to explain the measured island morphologies.<br />
Figure 1: Topographic NC-AFM images. (a) C60 island with dendritic second layer at LT. (b)<br />
and (c) represent the coexistence <strong>of</strong> compact triangular and branched islands at RT, with dendritic<br />
growth starting at the second layer (d).<br />
[1] S.A. Burke, J.M. Mativetsky, S. Fostner, P. Grütter, Phys. Rev. B 76, 035419 (2007)<br />
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