超顺磁性
顺磁性
布里渊函数和朗之万函数
凝聚态物理
铁磁性
材料科学
磁化
居里温度
单一领域
磁矩
磁性纳米粒子
磁各向异性
磁滞
磁滞
纳米颗粒
纳米技术
物理
磁场
量子力学
作者
Abdollah Hajalilou,Mahmoud Tavakoli,Elahe Parvini
标识
DOI:10.1002/9783527840762.ch11
摘要
A set of magnetic nanoparticles at different temperatures may have different magnetic states, including anisotropic superparamagnet, anisotropic superpromagnet, locked state, and super-spin glass and ferromagnetic glass phases. The superparamagnetism phenomenon is observed when the size of particles approaches to the single domain area in such a way that they behave as ferromagnetic materials below Curie temperature. Superparamagnetic (SPM) can be described based on the equations that are employed for paramagnetic particles, e.g. the Langevin function, with only a difference that the magnetic moment of individual particles is much larger in the case of SPM. Thus, the hysteresis loop, M–H or B–H, of SPM is more similar to that of a paramagnetic particle, but much steeper with higher magnetization. This is why they are named superparamagnetic.
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