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-10<br />
Transverse conductance image <strong>of</strong> DNA probed by current-feedback<br />
noncontact AFM<br />
T. Matsumoto 1, Y. Maeda 2, and T Kawai 1<br />
1 Institute <strong>of</strong> Scientific and Industrial Research (ISIR), Osaka Universit,Osaka, Japan<br />
2 National Institute <strong>of</strong> Advanced Industrial Science and Technology (AIST), Osaka Japan<br />
Scanning probe microscopy (SPM), which provides means to access to individual<br />
molecule, has a special significance for investigations <strong>of</strong> molecular-scale electronics. In<br />
particular, scanning tunneling microscopy (STM) has been used to evaluate molecular<br />
conductivity. However, STM measurement is effective only for height-foreknown system<br />
such as the molecules embedded in self-assembled monolayer. For the molecules having<br />
conformational variations, STM measurement is unable to separate the information <strong>of</strong><br />
transverse conduction through the molecules from the unknown height variation.<br />
We demonstrated that simultaneous measurement <strong>of</strong> tunnel current and frequency<br />
shift realized to separate electrical properties from topographic variations. Figure 1(a)<br />
shows simultaneously obtained STM topography (constant-current mode) and frequency<br />
shift image <strong>of</strong> DNA on Cu (111) surface. These images are totally similar to each other<br />
but the contrast distribution <strong>of</strong> these images shows differences. For the quantitative study<br />
<strong>of</strong> these variances, the correlation between STM height and frequency shift is analyzed by<br />
plotting each pixel as shown in Figure 2(a). The negative frequency shift overall increase<br />
as increasing STM height. This indicates that the tip close to the molecule at the high<br />
region <strong>of</strong> STM topography. Assuming the transverse electron tunneling through DNA<br />
molecules, frequency shift and STM height show linear relationship as a function <strong>of</strong><br />
transconductance G0 at molecule/surface interface and attenuation decay constant β. The<br />
line represented in Figure 2(a) means the data sets <strong>of</strong> STM height and frequency shift<br />
satisfying a parameter set <strong>of</strong> G0=0.27 and β= 0.26 . The pixel data picked from the plots<br />
around this line is used for reconstructing an image which shows a slice indicating the<br />
conduction with G0=0.27 and β= 0.26. As shown in Figure 2(b), the conductance image<br />
differ from either STM topography and frequency shift image in that it reflects the<br />
conductance variations affected by molecular conformation and/or molecules/substrate<br />
interface.<br />
STM topography Frequency shift image<br />
Fig. 1. Simultaneously obtained STM<br />
topography and frequency shift image<br />
<strong>of</strong> DNA on Cu (111).<br />
(a) Correlation analysis (b) Conductance image<br />
Frequency shift (Hz)<br />
4<br />
2<br />
0<br />
-2<br />
-4<br />
-6<br />
(G 0 ,β ) = (0.26, 0.27)<br />
-8<br />
-6 -4 -2 0 2 4 6 8<br />
STM height (nm)<br />
Fig. 2. (a) Correlation analysis between STM height<br />
and frequency. (b) Conductance image reconstructed<br />
from the data around the line <strong>of</strong> G0=0.27, β= 0.26.<br />
138