Nanoclustering phase competition induces the resistivity hump in colossal magnetoresistive manganites
arXiv:1711.10211 · doi:10.1103/PhysRevB.96.214416
Abstract
Using a two-band double-exchange model with Jahn-Teller lattice distortions and super-exchange interactions, supplemented by quenched disorder, at electron density , we explicitly demonstrate the coexistence of the = 1/2-type () charge-ordered and the ferromagnetic nanoclusters above the ferromagnetic transition temperature in colossal magnetoresistive (CMR) manganites. The resistivity increases due to the enhancement of the volume fraction of the charge-ordered and the ferromagnetic nanoclusters with decreasing the temperature down to . The ferromagnetic nanoclusters start to grow and merge, and the volume fraction of the charge-ordered nanoclusters decreases below , leading to the sharp drop in the resistivity. By applying a small external magnetic field , we show that the resistivity above increases, as compared with the case when , a fact which further confirms the coexistence of the charge-ordered and the ferromagnetic nanoclusters. In addition, we show that the volume fraction of the charge-ordered nanoclusters decreases with increasing the bandwidth and consequently the resistivity hump diminishes for large bandwidth manganites, in good qualitative agreement with experiments. The obtained insights from our calculations provide a complete pathway to understand the phase competition in CMR manganites.
6 pages, 6 figures
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