Abstract

Ca0.5Na0.5Cu2.5Mn4.5O12, CaCu3−xMn4+xO12 (0.5≤x≤2) were prepared at 700°C and 2600 PSI by combined sol–gel and high oxygen pressure methods. CaCu0.5Mn6.5O12 and CaMn7O12 (x=2.5 and 3) were prepared by solid state reactions in evacuated quartz tubes at 900°C. These compounds crystallize in a body-centered cubic variant of the perovskite structure except for CaMn7O12, which has rhombohedral symmetry. The oxidation states of Cu and Mn were investigated by X-ray absorption spectroscopy and chemical analysis. The oxidation state of Mn is near 4+ in Ca0.5Na0.5Cu2.5Mn4.5O12 and decreases with increasing x. Ca0.5Na0.5Cu2.5Mn4.5O12, CaCu2.5Mn4.5O12 (x=0.5), and CaCu1.5Mn5.5O12 (x=1.5) undergo a semiconductor-to-metal transition (TSM), CaCu2Mn5O12 (x=1.0) is metallic, while the 2.0≤x≤3.0 phases are semiconducting in the range 10–400 K. All of the materials (except the x=2.5 and 3.0) undergo a paramagnetic-to-ferromagnetic-like transition below their ordering temperatures (TC). The CaCu0.5Mn6.5O12 and CaMn7O12 (x=2.5 and 3.0) materials order antiferromagnetically at (TN) 40 and 20 K, respectively. The magnetic and resistivity results are summarized in a T–x phase diagram. The ordering temperatures decrease with increasing Mn3+ content, hence the double exchange mechanism does not appear to govern the ferromagnetic ordering. The highest magnetoresistance reaches a maximum of −32% for Ca0.5Na0.5Cu2.5Mn4.5O12 and is −28% for CaCu2.5Mn4.5O12 at 4.2 K and 5 T. In general, the magnetoresistance does not occur at the semiconductor-to-metal transition and it decreases smoothly with increasing temperature or x. These materials show high sensitivity of the magnetoresistance at low applied magnetic fields and good temperature stability of the magnetoresistance.

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