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Noncontact Atomic Force Microscopy - Yale School of Engineering ...

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We-1200<br />

<strong>Atomic</strong>-Resolution Damping <strong>Force</strong> Spectroscopy on Nanotube Peapods<br />

with Different Tube Diameters<br />

M. Ashino 1 , R. Wiesendanger 1 , A. N. Khlobystov 2 , S. Berber 3,4 , and D. Tománek 4<br />

1 Inst. <strong>of</strong> Applied Physics & Microstructure Research Center, University <strong>of</strong> Hamburg, Hamburg, Germany<br />

2 <strong>School</strong> <strong>of</strong> Chemistry, University <strong>of</strong> Nottingham, Nottingham, UK<br />

3 Physics Department, Gebze Institute <strong>of</strong> Technology, Gebze, Turkey<br />

4 Physics and Astronomy Department, Michigan State University, East Lansing, USA.<br />

Damping <strong>of</strong> the oscillating cantilever in dynamic atomic force microscopy (AFM)<br />

includes valuable information about the local vibrational structure and elastic compliance<br />

<strong>of</strong> the samples. We present atomically-resolved maps <strong>of</strong> damping in nanotube peapods,<br />

showing their capability <strong>of</strong> identifying the presence and location <strong>of</strong> encapsulated Dy@C82<br />

metall<strong>of</strong>ullerenes as well as their packing structure in the different diameters <strong>of</strong> carbon<br />

nanotubes. In our study, the physical origin <strong>of</strong> damping is elucidated in a microscopic<br />

model, and its relationship to the outer tube diameter is quantitatively interpreted by<br />

calculating the vibrational spectrum and energy dissipation in peapods with different<br />

diameters using ab initio total energy and molecular dynamics calculations [1].<br />

In our experiment we probed sparsely deposited (Dy@C82)@SWNT peapods on insulating<br />

oxide layers <strong>of</strong> a Si substrate by dynamic AFM under constant oscillation amplitude conditions in<br />

ultrahigh vacuum (p≈10 -8 Pa) and at low temperature (T≈13 K). As seen in Fig. 1(a), the<br />

atomically site-specific damping signal is obviously detected over the peapod. Besides,<br />

Figure 1(b) shows that its maximum energy is closely related to the enclosing nanotube<br />

diameter d, determined on the basis <strong>of</strong> the simultaneously observed topographic images.<br />

(a) (b)<br />

Figure 1: (a) Simultaneously obtained dynamic AFM topography (left) and damping (right)<br />

images <strong>of</strong> an empty SWNT (1,3) and a (Dy@C82)@SWNT peapod (2,4) with the same outer<br />

tube diameter d≈1.62 nm. (b) Relationship between outer tube diameter d and the maximum<br />

damping energy ΔEmax.<br />

[1] M. Ashino, R. Wiesendanger, A. N. Khlobystov, S. Berber, and D. Tománek,<br />

submitted for publication.<br />

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