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Introduction to Nanotechnology

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1.4<br />

N<br />

1 1.2 z<br />

" 1<br />

0<br />

v<br />

5<br />

h 0.8<br />

0<br />

0.6<br />

h<br />

E<br />

g 0.4<br />

0.2<br />

7.6. GIANT AND COLOSSAL MAGNETORESISTANCE 183<br />

B [10-'T]<br />

Figure 7.16. Dependence of the electrical resistance R(B), relative <strong>to</strong> its value R(0) in zero field,<br />

of a layered irowchromium system on a magnetic field B applied parallel <strong>to</strong> the surface of the<br />

layers. [Adapted from R. E. Camley, J. Phys. Condens. Matter 5, 3727 (1993).]<br />

nanoparticles parallel <strong>to</strong> the direction of the field, which reduces the resistance. The<br />

magnitude of the effect of the applied magnetic field on the resistance increases with<br />

the strength of the magnetic field and as the size of the magnetic nanoparticles<br />

decreases. Figure 7.18 shows a representative measurement at l00K of a film<br />

0 2 4 6 8 10 12 14 16 18 20<br />

THICKNESS OF Fe LAYER (nm)<br />

Figure 7.17. Dependence of the change of magne<strong>to</strong>resistance AR on the thickness of the iron<br />

magnetic layer in a constant DC magnetic field for the F 4 r layered system. [Adapted from<br />

R. E. Camley, J. Phys. Condens. Matter 5, 3727 (1993).]

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