Abstract

The conditions to obtain a table-like behavior of the entropy change, on the composite system $(LBMO_{2.98})_{1-x}/(LBMO_{2.95})_{x}$ , have been investigated from the isothermal magnetic entropy change versus temperature curves $ \Delta S(T)$ of La2/3Ba1/3MnO2.98 and La2/3Ba1/3MnO2.95 materials. The latters are characterized by Curie temperatures ( $ T_{C}$ ) values (310 K for La2/3Ba1/3MnO2.98 and 292 K for La2/3Ba1/3MnO2.95 around room temperature. The temperature dependence of the isothermal magnetic entropy change $\Delta S(T)$ has been calculated for the composite system with $ 0 \le x \le 1$ . The optimum magnetocaloric effect (MCE) properties, i.e., a $\Delta S(T)$ curve with table-like shape, have been found in the temperature interval of 293-309 K for the composite with $ x = 0.48$ at 1 T. The $\Delta S(T)$ of the composite comes close to a constant value of 1.73(7)J/(kg ·K). A large refrigerant capacity value of $\sim 66.4(9)$ J/kg is obtained in a wide temperature span over 16 K. This composite can be used as the working material in the Ericsson-cycle magnetic regenerative refrigerator. These results make the $(LBMO_{2.98})_{0.52}/(LBMO_{2.95})_{0.48}$ system a promising material for practical magnetic refrigeration using a lower field (1 T), which is much easier to generate by permanent magnets, than higher fields, like 2 T.

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