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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 />

147

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