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Phys. Rev. B 53, 14434–14444 (1996)

Intrinsic electrical transport and magnetic properties of La0.67Ca0.33MnO3 and La0.67Sr0.33MnO3 MOCVD thin films and bulk material

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G. Jeffrey Snyder
Department of Applied Physics, Stanford University, Stanford, California 94305-4090

Ron Hiskes and Steve DiCarolis
Hewlett-Packard, Palo Alto, California 94303-0867

M. R. Beasley and T. H. Geballe
Department of Applied Physics, Stanford University, Stanford, California 94305-4090

Received 22 September 1995; published in the issue dated 1 June 1996

An investigation designed to display the intrinsic properties of perovskite manganites was accomplished by comparing the behavior of bulk samples with that of thin films. Epitaxial 1500 Å films of perovskite La0.67Ca0.33MnO3 and La0.67Sr0.33MnO3 were grown by solid source chemical vapor deposition on LaAlO3 and post annealed in oxygen at 950 °C. Crystals were prepared by laser heated pedestal growth. The magnetic and electrical transport properties of the polycrystalline pellets, crystals, and annealed films are essentially the same. Below TC/2 the intrinsic magnetization decreases as T2 (as can be expected for itinerant electron ferromagnets) while the intrinsic resistivity increases proportional to T2. The constant and T2 coefficients of the resistivity are largely independent of magnetic field and alkaline earth element (Ca, Sr, or Ba). Hall effect measurements indicate that holes are mobile carriers in the metallic state. We identify three distinct types of negative magnetoresistance. The largest effect, observed near the Curie temperature, is 25% for the Sr and 250% [ΔR/R(H)] for the Ca compound. There is also magnetoresistance associated with the net magnetization of polycrystalline samples which is not seen in films. Finally a small magnetoresistance linear in H is observed even at low temperatures. The high temperature (above TC) resistivity of La0.67Ca0.33MnO3 is consistent with small polaron hopping conductivity with a slight transition at 750 K, while La0.67Sr0.33MnO3 does not exhibit activated conductivity until about 500 K, well above TC. The limiting low and high temperature resistivities place a limit on the maximum possible magnetoresistance of these materials and may explain why the "colossal" magnetoresistance reported in the literature correlates with the suppression of TC.

© 1996 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.53.14434
DOI:
10.1103/PhysRevB.53.14434
PACS: