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Introduction to Nanotechnology

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7.5. NANOCARBON FERROMAGNETS 179<br />

-8000 4ooo 0 4000 8000<br />

MAGNETIC FIELD (Oe)<br />

Figure 7.12. Magnetization curve hystersis loops for iron particles on the tips of aligned<br />

nanotubes at the temperatures of 5 and 320K, for a magnetic field H applied parallel <strong>to</strong> the<br />

tubes. An oersted corresponds <strong>to</strong> T. [Adapted from Z. Zhang et al., J. Magn. Magn. Mater.<br />

231, L9 (2001).]<br />

(4 K). These iron particles at the tips of aligned nanotubes could be the basis of high-<br />

density magnetic s<strong>to</strong>rage devices. The walls of the tubes can provide nonmagnetic<br />

separation between the iron nanoparticles, ensuring that the interaction between<br />

neighboring nanoparticles is not <strong>to</strong>o strong. If the interaction is <strong>to</strong>o strong, the fields<br />

required <strong>to</strong> flip the orientation would be <strong>to</strong>o large.<br />

'0 50 100 150 200 250 300 350<br />

TEMPERATURE (K)<br />

Figure 7.13. Plot of coercive field H, versus temperature T for iron particles on the tips of<br />

aligned nanotubes. A kilooersted corresponds <strong>to</strong> 0.1 T. [Adapted from Z. Zhang et al., J. Magn.<br />

Magn. Mater. 231, L9 (2001).]

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