Journal
PHYSICAL REVIEW B
Volume 66, Issue 10, Pages -Publisher
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.66.104416
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The phase change from a charge- and orbital-ordered insulator to a ferromagnetic metal has been investigated for single crystals of Pr-0.55(Ca1-ySry)(0.45)MnO3 with controlled one-electron bandwidth. At 0less than or equal toyless than or equal to0.2, the ground state is the charge- and orbital-ordered insulator, while for ygreater than or equal to0.25 it changes to a ferromagnetic metal. At around y=0.25, the critical temperatures for the charge-orbital ordering and the ferromagnetic transition coincide with each other (approximate to200 K), forming the bicritical point in the electronic phase diagram. Around this insulator-metal phase boundary, prototypical colossal magnetoresistance emerges in the metallic regime, while the charge-orbital ordering is melted by a relatively low magnetic field of a few tesla in the charge- and orbital-ordered insulating regime. The phase diagrams of Pr1-x(Ca1-ySry)(x)MnO3 (0less than or equal toyless than or equal to1) with various doping levels of x=0.35, 0.45, and 0.5 indicate that such a competition between the charge-orbital ordering and the ferromagnetic metal is critically dependent on the doping level. In particular, the commensurate doping level (x=0.5) tends to stabilize the charge- and orbital-ordered state even beyond the bicritical point in the lower-temperature side of the ferromagnetic phase.
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