Paramagnetic and Diamagnetic Susceptibility of Infinite Quantum Well

Adam B. Cahaya
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引用次数: 5

Abstract

Paramagnetism and diamagnetism of a material characterized by its magnetic susceptibility. When a material is exposed to an external magnetic field, magnetic susceptibility is defined as the ratio of the induced magnetization and the magnetic field. A paramagnetic material has magnetic susceptibility with positive sign. On the other hand, a diamagnetic material has magnetic susceptibility with negative sign. Atomically, paramagnetic materials consist of atoms that has orbital with unpaired electrons. Theoretical study of paramagnetic susceptibility and diamagnetic susceptibility are well described by Pauli paramagnetism and Landau diamagnetism, respectively. Although paramagnetism and diamagnetism are among the simplest magnetic properties of material that are studied in basic physics, theoretical derivations of Pauli paramagnetic and Landau diamagnetic susceptibility require second quantization formalism of quantum mechanics. We aim to discuss the paramagnetic and diamagnetic susceptibilities for simple three-dimensional quantum well using first quantization formalism.
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无限量子阱的顺磁性和抗磁性磁化率
以磁化率为特征的材料的顺磁性和抗磁性。当材料暴露在外磁场中时,磁化率定义为感应磁化强度与磁场的比值。顺磁性材料的磁化率为正号。反之,抗磁性材料的磁化率为负号。从原子的角度来说,顺磁性材料是由具有未配对电子轨道的原子组成的。泡利顺磁性和朗道抗磁性分别很好地描述了顺磁性和抗磁性的理论研究。虽然顺磁性和抗磁性是基础物理学中研究的最简单的材料磁性,泡利顺磁性和朗道抗磁性的理论推导需要量子力学的二次量子化形式。我们的目的是用第一量子化形式讨论简单三维量子阱的顺磁磁化率和反磁磁化率。
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