Haiou Wang, Fuxiao Dong, Haochen Wang, Bojun Zhao, Yan Wang, Weishi Tan
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The KF relation was suitable for the samples with x = 0.2 and 0.5, while the MAP method was suitable for the samples with x = 0.3 and 0.4. Among the Ising, XY, Heisenberg, and mean-field models, the samples with x = 0.2, 0.3, and 0.4 aligned more closely with the mean-field model, except for the x = 0.5 sample. Entropy change (−ΔSM) of Nd1−xSrxMnO3 (0.2 ≤ x ≤ 0.5) increased with the applied field, with the maximum value observed around TC. For the sample with x = 0.3, (−ΔSM) reached 4.315 J/kg K at μ0ΔH = 50 kOe, corresponding to a relative cooling power (RCP) of 280.48 J/kg. Remarkably, the x = 0.4 sample displayed (−ΔSM) of 3.298 J/kg K at μ0ΔH = 50 kOe near room temperature, with the RCP of 283.64 J/kg. These findings underscore the role of Sr doping in tuning the magnetic properties, critical behavior, and magnetocaloric effect of NdMnO3.","PeriodicalId":15088,"journal":{"name":"Journal of Applied Physics","volume":"16 1","pages":""},"PeriodicalIF":2.7000,"publicationDate":"2024-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Magnetic properties, critical behavior, and magnetocaloric effect of Nd1−xSrxMnO3 (0.2 ≤ x ≤ 0.5): The role of Sr doping concentration\",\"authors\":\"Haiou Wang, Fuxiao Dong, Haochen Wang, Bojun Zhao, Yan Wang, Weishi Tan\",\"doi\":\"10.1063/5.0229032\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Magnetic characteristics, magnetocaloric effect, and critical behavior of Nd1−xSrxMnO3 compounds by Sr doping (x = 0.2, 0.3, 0.4, 0.5) were studied. All samples maintained orthorhombic structures, but the space group changed from Pnma (No. 62) for x = 0.2, 0.3 to Imma (No. 74) for x = 0.4, 0.5. As Sr doping increased, the Curie temperature (TC), Curie–Weiss temperature (TCW), and magnetization increased, attributed to the double exchange (DE) interaction. A discrepancy between TCW and TC was observed due to the competition between polarons and DE interaction. The critical behavior was investigated systematically using the self-consistent (modified Arrott plots, MAP) method and the Kouvel–Fisher (KF) relation. The KF relation was suitable for the samples with x = 0.2 and 0.5, while the MAP method was suitable for the samples with x = 0.3 and 0.4. Among the Ising, XY, Heisenberg, and mean-field models, the samples with x = 0.2, 0.3, and 0.4 aligned more closely with the mean-field model, except for the x = 0.5 sample. 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引用次数: 0
摘要
研究了掺杂 Sr(x = 0.2、0.3、0.4、0.5)的 Nd1-xSrxMnO3 化合物的磁特性、磁致效应和临界行为。所有样品都保持正方体结构,但空间群从 x = 0.2、0.3 时的 Pnma(62 号)变为 x = 0.4、0.5 时的 Imma(74 号)。随着锶掺杂量的增加,居里温度(TC)、居里-韦斯温度(TCW)和磁化率也随之增加,这归因于双交换(DE)相互作用。由于极子和 DE 相互作用之间的竞争,观察到 TCW 和 TC 之间存在差异。利用自洽(修正阿罗特图,MAP)方法和库维尔-费舍(KF)关系对临界行为进行了系统研究。KF 关系适用于 x = 0.2 和 0.5 的样品,而 MAP 方法适用于 x = 0.3 和 0.4 的样品。在 Ising、XY、Heisenberg 和均场模型中,除 x = 0.5 样本外,x = 0.2、0.3 和 0.4 样本更接近均场模型。Nd1-xSrxMnO3(0.2 ≤ x ≤ 0.5)的熵变(-ΔSM)随施加的磁场而增加,在 TC 附近观察到最大值。对于 x = 0.3 的样品,在 μ0ΔH = 50 kOe 时,(-ΔSM) 达到 4.315 J/kg K,相当于 280.48 J/kg 的相对冷却功率 (RCP)。值得注意的是,x = 0.4 样品在接近室温的 μ0ΔH = 50 kOe 时显示出 3.298 J/kg K 的 (-ΔSM),相对冷却功率为 283.64 J/kg。这些发现强调了掺杂硒在调整 NdMnO3 的磁性能、临界行为和磁致效应方面的作用。
Magnetic properties, critical behavior, and magnetocaloric effect of Nd1−xSrxMnO3 (0.2 ≤ x ≤ 0.5): The role of Sr doping concentration
Magnetic characteristics, magnetocaloric effect, and critical behavior of Nd1−xSrxMnO3 compounds by Sr doping (x = 0.2, 0.3, 0.4, 0.5) were studied. All samples maintained orthorhombic structures, but the space group changed from Pnma (No. 62) for x = 0.2, 0.3 to Imma (No. 74) for x = 0.4, 0.5. As Sr doping increased, the Curie temperature (TC), Curie–Weiss temperature (TCW), and magnetization increased, attributed to the double exchange (DE) interaction. A discrepancy between TCW and TC was observed due to the competition between polarons and DE interaction. The critical behavior was investigated systematically using the self-consistent (modified Arrott plots, MAP) method and the Kouvel–Fisher (KF) relation. The KF relation was suitable for the samples with x = 0.2 and 0.5, while the MAP method was suitable for the samples with x = 0.3 and 0.4. Among the Ising, XY, Heisenberg, and mean-field models, the samples with x = 0.2, 0.3, and 0.4 aligned more closely with the mean-field model, except for the x = 0.5 sample. Entropy change (−ΔSM) of Nd1−xSrxMnO3 (0.2 ≤ x ≤ 0.5) increased with the applied field, with the maximum value observed around TC. For the sample with x = 0.3, (−ΔSM) reached 4.315 J/kg K at μ0ΔH = 50 kOe, corresponding to a relative cooling power (RCP) of 280.48 J/kg. Remarkably, the x = 0.4 sample displayed (−ΔSM) of 3.298 J/kg K at μ0ΔH = 50 kOe near room temperature, with the RCP of 283.64 J/kg. These findings underscore the role of Sr doping in tuning the magnetic properties, critical behavior, and magnetocaloric effect of NdMnO3.
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