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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 />

82

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