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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Theory <strong>of</strong> Multifrequency Method in FM-AFM<br />
Zongmin Ma, Yoshitaka Naitoh, Yanjun Li, Masami Kageshima<br />
and Yasuhiro Sugawara<br />
Department <strong>of</strong> Applied Physics, Graduate <strong>School</strong> <strong>of</strong> <strong>Engineering</strong>, Osaka University, 2-1 Yamada-oka,<br />
Suita, Osaka 565-0871, Japan<br />
P.I-29<br />
FM-AFM has been succeeded in measuring topography and energy dissipation<br />
with atomic resolution on the surface. Furthermore, force spectroscopy is<br />
demonstrated to identify the atomic species. The elasticity information <strong>of</strong> the surface<br />
is important physical information <strong>of</strong> the sample materials. Actually, it has been<br />
measured by using multifrequency method in AM-AFM recently, which was proposed<br />
by Rodriguez and Garcia and successfully demonstrated its usefulness theoretically<br />
and experimentally [1-2].<br />
In this paper, for the first time, we<br />
proposed usage <strong>of</strong> the multifrequency<br />
f 2<br />
BPF PLL Δf 2<br />
method in FM-AFM to measure the<br />
AGC<br />
sample properties such as elasticity.<br />
Figure 1 shows the block diagram <strong>of</strong><br />
×<br />
multifrequency method in FM-AFM.<br />
f 1<br />
BPF PLL<br />
The cantilever is excited simultaneously<br />
at the first and the second resonances.<br />
Band pass filters (BPFs) are used to<br />
separate the vibration signals <strong>of</strong> the<br />
Optical<br />
interferometer<br />
+<br />
+<br />
AGC<br />
×<br />
cantilever. For each signal, the cantilever<br />
Cantilever<br />
Δf 1<br />
is vibrated by self-oscillation at the first<br />
Feedback<br />
and the second resonances. Topography<br />
Tube Scanner<br />
Topography<br />
<strong>of</strong> the sample is obtained by the<br />
feedback signal to keep the frequency<br />
Figure 1. Block diagram <strong>of</strong> multifrequency<br />
shift (△ f1) constant. The elasticity information <strong>of</strong> the sample surface is measured by<br />
frequency shift (△ f2) <strong>of</strong> the second resonance, which is proportional to the<br />
conservative force between tip and sample. Here, we show the theory for the<br />
multifrequency method in FM-AFM.<br />
[1] Rodriguez and R. Garcia, Appl. Phys. Lett. 84, 449 (2004).<br />
[2] Jose R. Lozano and Ricardo Garcia. Phy Rev B 79, 014110 (2009).<br />
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