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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Th-1240 Fr-0900<br />
<strong>Atomic</strong> scale elasticity mapping <strong>of</strong> Ge(001) surface by multifrequency<br />
FM-AFM<br />
Yoshitaka Naitoh, Zongmin Ma, Yanjun Li, Masami Kageshima and Yasuhiro Sugawara<br />
Department <strong>of</strong> Applied Physics, Osaka University, Suita 565-0871, JAPAN<br />
Surface elasticity is quite important to study atomic scale properties <strong>of</strong> the surface<br />
such as bounding strength <strong>of</strong> surface atoms and surface phonons. The conventional FM-<br />
AFM provides topographic information <strong>of</strong> various surfaces at atomic scale. However, it is<br />
hardly accessible to the elasticity and the adhesion on surfaces. In this study, we propose<br />
a new technique, multifrequency FM-AFM, on Ge(001) surface using a commercial<br />
cantilever in order to investigate the surface elasticity at atomic scale with the<br />
topographic image.<br />
The cantilever <strong>of</strong> the multifrequency FM-AFM was simultaneously excited at the<br />
by two sets <strong>of</strong> automatic gain<br />
1st and the 2nd flexural resonant frequencies (f1st, f2nd)<br />
controller and phase locked loop electronics. Their oscillating amplitudes are set constant<br />
at A1st, A2nd. The cantilever oscillating signal, detected by an optical interferometer<br />
system, is divided into the 1st and the 2nd components through band pass filters. The<br />
surface topography is obtained from feedback signal maintaining the frequency shift <strong>of</strong><br />
the 1st component (Δf1st) constant. From the theoretical consideration, we found that the<br />
surface elasticity is obtained as a mapping <strong>of</strong> the frequency shift <strong>of</strong> the 2nd component<br />
(Δf2nd).<br />
The cleaned Ge(001) surface showing buckled dimer structure was adopted as a<br />
sample with the elastic distribution at atomic scale. Figures 1(a) and (b) show the<br />
simultaneously obtained topography and the Δf2nd mapping <strong>of</strong> the surface. The dimer<br />
structure <strong>of</strong> the surface was clearly resolved in both images. We found Δf2nd <strong>of</strong> the fig.<br />
1(b) was high at the dimer atom position in comparison with the topography. This result<br />
suggests multifrequency FM-AFM is a nicer tool for exploring the surface elasticity at<br />
atomic scale.<br />
Figure 1: (a) Topographic image <strong>of</strong> Ge(001) surface with Δf1st=-70Hz, f1st=160kHz and<br />
A1st=4nm. Scan area is 7x7 nm 2 . (b) Simultaneously obtained Δf2nd mapping <strong>of</strong> the surface area<br />
with Δf2nd=-21Hz, f2nd=1.0MHz and A2nd=0.3nm.<br />
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