Abstract

The insulator-metal transition in single crystal ${\mathrm{La}}_{5/8\ensuremath{-}y}{\mathrm{Pr}}_{y}{\mathrm{Ca}}_{3/8}{\mathrm{MnO}}_{3}$ with $y\ensuremath{\approx}0.35$ was studied using synchrotron x-ray diffraction, electric resistivity, magnetic susceptibility, and specific heat measurements. Despite the dramatic drop in the resistivity at the insulator-metal transition temperature ${T}_{\mathrm{MI}},$ the charge-ordering (CO) peaks exhibit no anomaly at this temperature and continue to grow below ${T}_{\mathrm{MI}}.$ Our data suggest then, that in addition to the CO phase, another insulating phase is present below ${T}_{\mathrm{CO}}.$ In this picture, the insulator-metal transition is due to the changes that occur within this latter phase. The CO phase does not appear to play a major role in this transition. We propose that a percolationlike insulator-metal transition occurs via the growth of ferromagnetic metallic domains within the parts of the sample that do not exhibit charge ordering. Finally, we find that the low-temperature phase-separated state is unstable against x-ray irradiation, which destroys the CO phase at low temperatures.

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