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MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

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100 Chapter 4<br />

above room temperature, but the effect decreases significantly with<br />

temperature.<br />

Three regions of magnetoresistance are identified in these materials. The<br />

largest effect is likely due to the suppression of magnetic critical scattering<br />

near the Curie temperature. There is also a negative magnetoresistance<br />

associated with the net magnetization of polycrystalline samples but not seen<br />

in single crystal materials. Finally there is a small negative<br />

magnetoresistance linear in field even at low temperatures.<br />

The compounds La 0.67 Ca 0.33 MnO 3 and La 0.67 Sr 0.33 MnO 3 are metallic<br />

ferromagnets with large saturation moments. The saturation magnetization<br />

is found to decrease proportional to T 2 .<br />

The high temperature resistivity of La 0.67 Ca 0.33 MnO 3 clearly follows the law<br />

predicted by small polaron hopping conductivity both in the thermally<br />

activated regime and at higher temperatures where scattering becomes<br />

important. There appears to be a structural transition at about 750K.<br />

The resistivity of La 0.67 Sr 0.33 MnO 3 above the Curie temperature shows a<br />

crossover from a metallic to a hopping regime at higher temperatures.<br />

In conclusion, the CMR effects in materials of the same compositions as<br />

those studied here but with much lower transition temperatures, are not<br />

intrinsic to the thermodynamically stable phase. Local inhomogeneities or<br />

noncrystallinity in not fully annealed films may suppress the magnetic and<br />

metal-insulator transitions. This presumably causes the observed<br />

superparamagnetic type magnetism and conduction via percolation.

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