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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P.II-19<br />
Cantilever Holder Design for Spurious-Free Cantilever Excitation in<br />
Hitoshi Asakawa 1 and Takeshi Fukuma 1,2<br />
Liquid by Piezoactuator<br />
1 Frontier Science Organization, Kanazawa University, Japan<br />
2 PRESTO, JST, Japan<br />
Recent advancement in frequency modulation atomic force microscopy (FM-AFM)<br />
has enabled us to obtain atomic and molecular resolution images in liquid, which has<br />
encouraged us to explore the possibilities <strong>of</strong> FM-AFM application in biological research.<br />
In liquid-environment FM-AFM, a method for cantilever excitation is particularly<br />
important for ensuring the stability and accuracy in imaging and quantitative force<br />
measurements. This is because FM-AFM utilizes a cantilever deflection signal not only<br />
for obtaining a distance feedback signal (i.e., frequency shift signal) but also for<br />
producing a cantilever excitation signal. Although the cantilever excitation with a<br />
piezoactuator is most commonly used, the method typically results in an excitation <strong>of</strong><br />
spurious resonances around the natural resonance frequency <strong>of</strong> a cantilever due to the<br />
uncontrolled propagation <strong>of</strong> acoustic waves from a piezoactuator to the cantilever (Fig.<br />
1(a)).<br />
In order to suppress the influence <strong>of</strong> the spurious resonances, we propose a cantilever<br />
holder design, where the propagation <strong>of</strong> an acoustic wave is restricted the surrounding<br />
boundaries between two materials having significantly different specific acoustic<br />
resistances (ρ·c [kg/m 2 ·s]). In our design, an acoustic wave is greatly reduced by the<br />
reflection at the boundary between a piezoactuator (PZT, ρ·c=35×10 6 ) and its supporting<br />
material (PEEK, ρ·c=3.3×10 6 ). Then the remaining acoustic wave is further reduced by<br />
the reflection at the boundaries between the PEEK part and other components such as a<br />
cantilever support (stainless steel 316, ρ·c=36×10 6 ) and an optical window (glass,<br />
ρ·c=11×10 6 ). Figure 1 demonstrates the remarkable effect <strong>of</strong> the acoustic boundaries for<br />
suppressing spurious vibrations induced by the acoustic waves.<br />
a) b)<br />
Figure 1: Frequency responses <strong>of</strong> cantilever oscillation amplitude induced by a piezoactuator.<br />
(Excitation amplitude, : 0.5 V, : 1 V, : 1.5 V). Supporting materials for a piezoactuator: (a)<br />
stainless steel 316 and (b) PEEK.<br />
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