安德森晶格模型零场电子比热的变分理论:在巨磁阻锰矿(Re1-xAxMnO3)中的应用

S. Panwar, I. Singh
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引用次数: 0

摘要

使用简单的变分方法,我们研究了零场电子比热(Cv)作为安德森晶格模型温度的函数,用于掺杂碱土的稀土锰(Re=La, Pr, Nd等,a = Ca, Sr, Ba等),其表现出巨大的磁阻(CMR),金属绝缘体转变和许多其他鲜为人知的现象。我们已经用这种变分方法研究了掺杂CMR锰矿石的电阻率和磁化率等零场电子磁性能。我们采用强电子晶格JahnTeller (JT)耦合体系中锰的两波段(l-b) Anderson晶格模型哈密顿量来研究C在这些化合物中的温度依赖性。我们还观察到模型参数的作用,例如局部库伦斥力u,强铁磁洪德规则耦合eg和t2g自旋之间的JH以及相同自旋的l极化子和d电子之间的杂化Vk对Cv和线性系数Cv/T的作用。我们从我们的结果中发现,当温度降低到临界温度Tc(˷100 K)以下时,Cv(T)和Cv/T都有一个异常(尖峰),超过该异常(尖峰),JH的特定值会下降。V和掺杂值x与许多CMR化合物La0.815 Sr0.185 MnO3和Pr0.6-xBixSr0.4MnO3的关键特征相似(x= 0.00.15)。随着Vk或JH或掺杂x值的增加,观察到的Cv(T)低温峰逐渐变宽,并向更高的温度区域移动。在Tc˷100 K附近的比热异常与顺磁铁磁跃迁和磁不均匀性引起的磁有序有关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A variational theory of zero field electronic specific heat of Anderson lattice model: An application to colossal magnetoresistive manganites (Re1-xAxMnO3)
Using a simple variational method, we have studied the zero field electronic specific heat (Cv) as a function of temperature of Anderson lattice model used for rare earth manganites doped with alkaline earths namely ( where Re=La, Pr, Nd etc., and A= Ca, Sr, Ba etc.) which exhibit colossal magnetoresistance (CMR), metalinsulator transition & many other poorly understood phenomena . We have already used this variational method to study the zero field electronic & magnetic properties like electrical resistivity & magnetic susceptibility of doped CMR manganites. We have taken two band (l-b) Anderson lattice model Hamiltonian for manganites in the strong electronlattice JahnTeller (JT) coupling regime to study the temperature dependence of C vin these compounds. We have also observed the role of the model parameters e.g. local Coulomb repulsionU, strong ferromagnetic Hund’s Rule coupling JH between eg& t2g spins & hybridization Vk between l– polarons& d electrons of the same spins on Cv&linear coefficient Cv/ T. We find from our results that as the temperature is lowered below a critical temperature Tc (˷100 K), there is an anomaly (sharp peak) in both Cv(T) &Cv/T beyond which it falls off for particular values of JH, V & doping values x resembling with the key feature of many CMR compounds La0.815 Sr0.185 MnO3 & Pr0.6-xBixSr0.4MnO3(x= 0.00.15). The observed low temperature peak in Cv(T) becomes progressively broader & shifts to higher temperature region on increasing Vk or JH or doping x value. The specific heat anomaly near Tc ˷ 100 K is related to magnetic ordering due to the paramagneticferromagnetic transitions and magnetic inhomogeneity in these manganites.
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