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Introduction to Nanotechnology

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182 NANOSTRUCTURED FERROMAGNETISM<br />

NON MAGNETIC METAL<br />

NON MAGNETIC METAL<br />

0<br />

NiFe 4<br />

Figure 7.15. Three arrangements for producing colossal magne<strong>to</strong>resistance: (a) layers of<br />

nonmagnetic material alternating with oppositely magnetized (arrows) ferromagnetic layers;<br />

(b) randomly oriented ferromagnetic cobalt nanoparticles (large circles) in a nonmagnetic copper<br />

matrix (small circles); (c) hybrid system consisting of cobalt nanoparticles in a silver (Ag) matrix<br />

sandwiched between nickeliron (NiFe) magnetic layers, with alternating magnetizations<br />

indicated by arrows.<br />

The magne<strong>to</strong>resistance effect in these layered materials is a sensitive detec<strong>to</strong>r of<br />

DC magnetic fields, and is the basis for the development of a new, more sensitive<br />

reading head for magnetic disks. Prior <strong>to</strong> this, magnetic s<strong>to</strong>rage devices have used<br />

induction coils <strong>to</strong> both induce an alignment of the magnetization in a small region of<br />

the tape (write mode), and <strong>to</strong> sense the alignment of a recorded area (read mode).<br />

The magne<strong>to</strong>resistive reading head is considerably more sensitive than the inductive<br />

coil method.<br />

Materials made of single-domain ferromagnetic nanoparticles with randomly<br />

oriented magnetizations embedded in a nonmagnetic matrix also display giant<br />

magne<strong>to</strong>resistance. Figure 7.15b shows a schematic of this system. The magne<strong>to</strong>-<br />

resistance in these materials, unlike the layered materials, is isotropic. The applica-<br />

tion of the DC magnetic field rotates the magnetization vec<strong>to</strong>r of the ferromagnetic

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