Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Fr-1220<br />
Redox-state Dependent Reversible Change <strong>of</strong> Molecular Ensembles in<br />
Water Solution by Electrochemical FM-AFM<br />
Ken-ichi Umeda 1† , Yasuyuki Yokota 2 , and Ken-ichi Fukui 2,3<br />
1 Department <strong>of</strong> Chemistry, Tokyo Institute <strong>of</strong> Technology, Tokyo, Japan.<br />
2 Department <strong>of</strong> Materials <strong>Engineering</strong> Science, Osaka University, Osaka, Japan.<br />
3 PRESTO, Japan Science and Technology Agency, Saitama, Japan.<br />
Electrochemisty can provide wide range <strong>of</strong> science and technology because <strong>of</strong> easy<br />
control <strong>of</strong> electrochemical potentials <strong>of</strong> interfaces and adsorbed molecules, which initiate<br />
electron transfer and chemical reactions hard to achieve in vacuum. Redox-active<br />
molecules fixed on the electrode can reversibly change their charges depending on the<br />
electrode potential, which makes it possible to introduce a point charge at the<br />
electrode/solution interface. Following the recipe in literature to reduce the deflection<br />
noise density in liquid-phase measurements, we have developed a frequency-modulation<br />
AFM applicable in electrochemical environments with controlling the potential <strong>of</strong> the tip<br />
and the sample. By using the EC-FM-AFM, we have studied how the charging <strong>of</strong> the<br />
molecule fixed at the electrode/solution interface affect the local structure.<br />
Ferrocenylundecanethiol (FcC11H22SH) molecules were embedded in an n-decanethiol<br />
(C10H21SH) self-assembled monolayer (SAM) matrix as molecular islands In Figure 1(a),<br />
the Fc-islands are shown as bright protrusions, whose apparent height differ depending<br />
on their lateral size (number <strong>of</strong> involved molecules). By changing the charge <strong>of</strong> Fcterminal<br />
groups from Fc 0 to Fc +1 , the apparent height and the lateral size <strong>of</strong> each Fcisland<br />
has clearly increased as shown in Figure 1(b). The process was reversible against<br />
the potential change, and originated from the change in the local charge. Simultaneously<br />
obtained energy dissipation signal has decreased at the island when the Fc-islands had<br />
positive charge. These results can be reasonably explained by the formation <strong>of</strong> ion<br />
network from Fc + and ClO4 - counter anions supplied from the electrolyte water solution.<br />
(a) Fc (b) 0<br />
Fc +1<br />
Figure 1: In situ EC-FM-AFM images (Δƒ = +528 Hz) <strong>of</strong> FcC11H22SH islands embedded in<br />
C10H21SH SAM (200×160 nm 2 50 nm 50 nm<br />
) at different electrochemical potentials: (a) substrate potential (Es)<br />
= tip potential (Et) = -0.8 V, (b) Es = Et = -0.4 V vs. Au/AuOx, respectively. The amplitude <strong>of</strong><br />
cantilever vibration was maintained in a feedback loop to be 0.5 nm.<br />
†<br />
Present address: Department <strong>of</strong> Electronic Science and <strong>Engineering</strong>, Kyoto University, Japan.<br />
90