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Introduction to Nanotechnology

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122 CARBONNANOSTRUCTURES<br />

magne<strong>to</strong>resistance effect because the resistance decreases with increasing DC<br />

magnetic field, so its reciprocal, the conductance G = 1 /R, increases. This occurs<br />

because when a DC magnetic field is applied <strong>to</strong> the nanotubes, the conduction<br />

electrons acquire new energy levels associated with their spiraling motion about<br />

the field. It turns out that for nanotubes these levels, called Landau levels, lie very<br />

close <strong>to</strong> the <strong>to</strong>pmost filled energy levels (the Fermi level). Thus there are more available<br />

states for the electrons <strong>to</strong> increase their energy, and the material is more conducting.<br />

5.4.4. Vibrational Properties<br />

The a<strong>to</strong>ms in a molecule or nanoparticle continually vibrate back and forth. Each<br />

molecule has a specific set of vibrational motions, called normal modes of vibration,<br />

which are determined by the symmetry of the molecule For example carbon dioxide<br />

C02, which has the structure O=C=O, is a bent molecule with three normal modes.<br />

One mode involves a bending of the molecule. Another, called the symmetric<br />

stretch, consists of an in-phase elongation of the two C=O bonds. The asymmetric<br />

A,g 165 cm-’<br />

E, 17 cm-’<br />

Figure 5.19. Illustration of two normal modes of vibration of carbon nanotubes

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