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Nanotechnology-Enabled Sensors

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6.7 Magnetically Engineered Spintronic <strong>Sensors</strong> 359<br />

Fig. 6.49 GMR results from interfacial spin-polarized scattering between ferromagnets<br />

separated by conducting spacers in a heterogeneous magnetic material,<br />

such as a magnetic multilayer or granular alloy. Reprinted with permission from<br />

the IEEE publications. 115<br />

As was mentioned previously, one of the largest GMR effects at room<br />

temperature is approximately 100%, which has been found in sputter deposited<br />

Co/Cu multilayers. 122 The thinner the magnetic and nonmagnetic<br />

layers are the larger the GMR effect will be as the GMR effect is dominated<br />

by spin-dependent scattering at magnetic/nonmagnetic interfaces. 123<br />

Thickening these layers largely results in shunting of current away from<br />

the interfacial regions. 124<br />

Manganese oxides with a perovskite structure exhibit a transition between<br />

a paramagnetic insulating phase and a ferromagnetic metal phase. 125<br />

Colossal magnetoresistance (CMR) is associated with this transition which<br />

was reported by Jin et al in 1993-1994. 126 In the vicinity of the transition<br />

temperature, such materials exhibit a large change in resistance in response<br />

to an applied magnetic field. CMR has not been explained by any current<br />

physical theories and is currently the focus of ongoing research. CMR

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