Abstract
The system RCaCrO4 (R Y, Sm, Pr) presents an orthorhombic structure (space group Bmab) at room temperature (RT), similar to that observed in La2MO4 (M Cu, Ni, Co). The magnetic susceptibility for RCaCrO4 shows a weak temperature dependence down to 250 K, probably due to the antiferromagnetic ordering of the Cr sublattice above RT. Below RT there is a strong upturn anomaly at 210, 190 and 130 K for Pr, Sm and Y, respectively. This anomaly is associated with the appearance of a weak ferromagnetic component, and could be related to a low temperature structural phase transition, similar to that observed in the related compounds R2NiO4 or La1.88Ba0.12CuO4. In the case of YCaCrO4 this ferromagnetic component produces a hysteresis curve at 4.5 K with a coercive field of 0.7 T. For PrCaCrO4 the coercive field is very small (< 0.05 T). SmCaCrO4 shows a more complicated behavior with a low temperature magnetic transition (TN2 ≈ 40 K), which could be associated with either the antiferromagnetic ordering of the Sm sublattice or a spin reorientation in the Cr sublattice.
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