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Above Room Temperature Magnetocaloric Effect In Perovskite Pr_(0.6)sr_(0.4)mno_3

机译:钙钛矿Pr_(0.6)sr_(0.4)mno_3的室温磁热效应

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The dependence of magnetization M on the applied magnetic field H and temperature T was measured carefully, near the Curie temperature T_c for the perovskite manganite sample Pr_(0.6)Sr_(0.4)MnO_3. The experimental results indicate that this specimen exhibit ferromagnetic (FM) to paramagnetic (PM) transition at T_c~320 K. In the 200 K-45 K temperature range the spontaneous magnetization was decreasing, probably due to spin canted state between manganese and praseodymium spin systems. At 46 K the magnetization presents a second little transition, which can be ascribed to very weak traces of secondary Mn_3O_4 phase, and remains constant between 10 K and 46 K. The maximum value of the magnetic entropy change obtained from the M(H) plot data is |ΔS_M~(max)| = 2.3 Jkg~(-1) K~(-1) for applied magnetic field of 2.5 T. At this value of magnetic field the relative cooling power (RCP) is 34.5 Jkg~(-1). The temperature corresponding to ΔS_M maximum value is almost equal to T_c. The large entropy change can be attributed to the fact that the ferromagnetic transition enhances the effect of the applied magnetic field greatly. It is suggested by the results that this compound can be used as the working material in an active magnetic regenerative refrigerator above room temperature.
机译:在钙钛矿锰矿样品Pr_(0.6)Sr_(0.4)MnO_3的居里温度T_c附近,仔细测量了磁化强度M对施加磁场H和温度T的依赖性。实验结果表明,该试样在T_c〜320 K时表现出铁磁(FM)至顺磁(PM)的转变。在200 K-45 K的温度范围内,自发磁化强度下降,这可能是由于锰和ase自旋之间的自旋倾斜状态造成的。系统。在46 K时,磁化强度呈现第二个小跃迁,这可以归因于次级Mn_3O_4相的非常微弱的痕迹,并且在10 K和46 K之间保持恒定。从M(H)图获得的磁熵变的最大值数据为|ΔS_M〜(max)|对于施加的2.5 T磁场= 2.3 Jkg〜(-1)K〜(-1)。在该磁场值下,相对冷却功率(RCP)为34.5 Jkg〜(-1)。对应于ΔS_M最大值的温度几乎等于T_c。较大的熵变化可归因于铁磁跃迁大大增强了施加磁场的效果。结果表明,该化合物可用作室温以上的有源磁蓄冷器中的工作材料。

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