皮帕德关系式应用于电介质和磁性材料中的某些跃迁

P. Wright
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引用次数: 7

摘要

当对居里点或尼尔点附近的行为进行基于热力学的比较时,Pippard的关系原则上比Ehrenfest的更相关。在对Sawatzky和Bloom(1962-64)和Skalyo, Cohen, Friedberg和Griffiths(1967)的分析进行补充的讨论中,考虑了各种磁Pippard关系,需要再次强调的是,Fisher(1960-62)在统计力学方面推导出的关系(在反铁磁尼尔点附近,比热的上升与磁化率的温度系数密切相关)非常接近于Pippard在lambda跃迁中一般得到的纯热力学类型的关系。用这种术语分析了一些有代表性的情况下的相关观测结果,并与λ温度对静水压力和磁场的依赖关系进行了比较。相应地,对于介电性质随温度变化非常快的λ跃迁,λ温度对应于磁化率对温度导数的峰值,而不是磁化率本身的最大值。
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Pippard's relations applied to certain lambda transitions in dielectric and magnetic materials
When making thermodynamically based comparisons concerning behaviour in the vicinity of Curie points or Neel points, Pippard's relations are in principle more pertinent than Ehrenfest's. In a discussion supplementing the analyses of Sawatzky and Bloom (1962-64) and Skalyo, Cohen, Friedberg and Griffiths (1967), various magnetic Pippard's relations are considered, and it is re-emphasized that a relation derived by Fisher (1960-62) in statistical mechanical terms (that near an antiferromagnetic Neel point the rise in specific heat closely follows the temperature coefficient of the magnetic susceptibility) amounts very nearly to a relation of the purely thermodynamic type obtained by Pippard for lambda transitions generally. Relevant observations are analyzed in such terms for a number of representative cases, and comparisons made with the dependence of lambda temperatures on hydrostatic pressure and magnetic field. Correspondingly, for lambda transitions associated with a very rapid change of dielectric properties with temperature, the lambda temperature corresponds to a peak in the derivative of electric susceptibility with respect to temperature, and not to a maximum in the susceptibility itself.
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