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Estimating spontaneous magnetization from a mean field analysis of the magnetic entropy change

机译:从磁熵变化的平均场分析估算自发磁化

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The magnetocaloric effect is a common property of all magnetic systems, corresponding to a temperature change under adiabatic conditions (ΔT_(ad)) or a change in magnetic entropy in isothermal conditions (ΔS_M), for a given applied magnetic field change. ΔT_(ad) can be directly measured under adiabatic conditions and indirectly estimated from specific heat measurements. ΔS_M can be indirectly estimated from specific heat measurements or magnetization measurements (the usual approach). Early work on the study of ferromagnets used direct measurements of ΔT_(ad) to determine the spontaneous magnetization for a given temperature value. In this work, we use ΔS_M obtained from isothermal magnetization measurements to estimate the spontaneous magnetization, comparing this result to mean-field fittings from a novel scaling method, discussing the validity and usefulness of this approach from considerations from the Landau theory of phase transitions.
机译:磁热效应是所有磁性系统的常见性,对应于绝热条件下的温度变化(Δt_(Δt_(ad))或等温条件(Δs_m)中的磁熵的变化,用于给定的施加的磁场变化。 ΔT_(AD)可以直接在绝热条件下测量,并从特定的热测量间接估计。可以从特定的热测量或磁化测量(通常的方法)间接地估计ΔS_M。关于铁磁体研究的早期工作使用ΔT_(AD)的直接测量来确定给定温度值的自发磁化。在这项工作中,我们使用从等温磁化测量中获得的ΔS_m来估计自发磁化,从新颖的缩放方法比较这一结果与平均缩放方法的平均配件,讨论了这种方法的有效性和有用性,从阶段转型的地兰理论的考虑中的考虑因素。

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