Regulation of Magnetic Phase Transition and Magnetocaloric Effect of DyCo2−xCrx Compounds
Wang Chen, Lei Ma, Shifan Lu, Jiacai Xiong, Lin Li, Jiang Wang, Guanghui Rao
Abstract
Wang Chen, Lei Ma, Shifan Lu, Jiacai Xiong, Lin Li, Jiang Wang, Guanghui Rao
Abstract
The magnetic phase transition, magnetic and magnetocaloric effect of DyCo2−xCrx (x = 0.0–0.2) compounds have been studied. X‐ray diffraction (XRD) data show that the main phases of DyCo2−xCrx compounds are MgCu2‐type cubic crystal structure, and the maximum atomic concentration of Cr in DyCo2 is 5%. With the x changed from 0.0 to 0.2, both of the lattice parameter and cell volume increased, and the coercivity at 10 K increased from 890 to 2839 Oe. With the introduction of Cr atoms, the type of magnetic phase transition can be regulated from the first order to the second order. Under a 5 T magnetic field, the maximum magnetic entropy changes (ΔSM) of DyCo2−xCrx (x = 0.0, 0.1, and 0.2) compounds are 10.4, 8.4, and 6.8 J kg−1 K−1, respectively, but the relative cooling power (RCP) actually increases, with values of 290.6, 312.5, and 396.7 J kg−1 respectively, which is because the width at half‐maximum of the ΔSM peak (δTFWHM) is increased.
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The magnetic phase transition, magnetic and magnetocaloric effect of DyCo2−xCrx (x = 0.0–0.2) compounds have been studied. X‐ray diffraction (XRD) data show that the main phases of DyCo2−xCrx compounds are MgCu2‐type cubic crystal structure, and the maximum atomic concentration of Cr in DyCo2 is 5%. With the x changed from 0.0 to 0.2, both of the lattice parameter and cell volume increased, and the coercivity at 10 K increased from 890 to 2839 Oe. With the introduction of Cr atoms, the type of magnetic phase transition can be regulated from the first order to the second order. Under a 5 T magnetic field, the maximum magnetic entropy changes (ΔSM) of DyCo2−xCrx (x = 0.0, 0.1, and 0.2) compounds are 10.4, 8.4, and 6.8 J kg−1 K−1, respectively, but the relative cooling power (RCP) actually increases, with values of 290.6, 312.5, and 396.7 J kg−1 respectively, which is because the width at half‐maximum of the ΔSM peak (δTFWHM) is increased.
Key concepts: Magnetic refrigeration, Coercivity, Full width at half maximum, Materials science, Phase transition, Condensed matter physics, Diffraction, Magnetic field