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Introduction to Nanotechnology

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86 PROPERTIES OF INDIVIDUAL NANOPARTICLES<br />

e<br />

e e<br />

I I I I I I I 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1<br />

Figure 4.14. Reaction rate of hydrogen gas with iron nanoparticles versus the particle size.<br />

[Adapted from R. L. Whetten et al., Phys. Rev. Lett. 54, 1494 (1985).]<br />

4.2.6. Fluctuations<br />

Very small nanoparticles, as is clear from the sketches in Figs. 4.6 and 4.8, have all<br />

or almost all of their a<strong>to</strong>ms on the surface. Surface a<strong>to</strong>ms are less restricted in their<br />

ability <strong>to</strong> vibrate than those in the interior, and they are able <strong>to</strong> make larger<br />

excursions from their equilibrium positions. This can lead <strong>to</strong> changes in the structure<br />

of the particle. Observations of the changes in the geometry with time of gold clusters<br />

have been made using an electron microscope. The gold clusters of 1CrlOO-8, radii<br />

are prepared in vacuum and deposited on a silicon substrate, which is then covered<br />

with an SiOz film. The electron microscope pictures of gold nanoparticles presented<br />

in Fig. 4.15, which were taken at different times, show a number of fluctuation-<br />

induced changes in the structure brought about by the particles transforming<br />

between different structural arrangements. At higher temperatures these fluctuations<br />

can cause a breakdown in the symmetry of the nanoparticle, resulting in the<br />

formation of a liquid-like droplet of a<strong>to</strong>ms.<br />

4.2.7. Magnetic Clusters<br />

Although it is not rigorously correct and leads <strong>to</strong> incorrect predictions of some<br />

properties, an electron in an a<strong>to</strong>m can be viewed as a point charge orbiting the<br />

nucleus. Its motion around the nucleus gives it orbital angular momentum and<br />

produces a magnetic field (except for s states). The magnetic field pattern arising<br />

from this movement resembles that of a bar magnet. The electron is said <strong>to</strong> have an<br />

orbital magnetic moment. There is also another contribution <strong>to</strong> the magnetic moment<br />

arising from the fact that the electron has a spin. Classically one can think of the<br />

electron as a spherical charge rotating about some axis. Thus there is both a spin and<br />

an orbital magnetic moment, which can be added <strong>to</strong> give the <strong>to</strong>tal magnetic<br />

e.

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