La1−xCaxCrO3中反铁磁绝缘体-铁磁半金属-反铁磁金属转变的开始及其微观起源

Jeel Swami, A. Dixit, B. Tiwari
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引用次数: 1

摘要

研究了LaCrO3和CaCrO3固溶体在完全混相范围内的磁基态,即在x = 0.25区间内,La1−xCaxCrO3的磁基态为0≤x≤1,以了解随Ca取代分数的磁相变。密度泛函理论与哈伯德校正用于解释Cr交换相互作用。等结构La1−xCaxCrO3体系表现出反铁磁绝缘体(x = 0,即LaCrO3)到铁磁半金属(x = 0.75,即La0.25Ca0.75CrO3)到反铁磁金属(x = 1,即CaCrO3)的相变。Cr的氧化态由LaCrO3中的3+变为CaCrO3中的4+,中间组分同时呈现3+和4+状态。有趣的是,引入Hubbard能量U和Ca取代会影响Cr-O杂化,正如在部分态密度中观察到的那样。给出了La1−xCaxCrO3(0≤x≤1)体系具有磁性基态的组成相图。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Onset of Antiferromagnetic Insulator‐to‐Ferromagnetic Half Metal‐to‐Antiferromagnetic Metal Transitions in La1−xCaxCrO3 and their Microscopic Origin
The magnetic ground state of LaCrO3 and CaCrO3 solid solution is investigated in the complete miscibility range, that is, La1−xCaxCrO3 with 0 ≤ x ≤ 1 at the interval of x = 0.25 to understand the magnetic phase transitions with Ca substitutional fraction. The density functional theory is used with Hubbard correction to account for Cr exchange interaction. The isostructural La1−xCaxCrO3 system exhibits antiferromagnetic insulator (x = 0, i.e., LaCrO3) to ferromagnetic half metal (x = 0.75, i.e., La0.25Ca0.75CrO3) to antiferromagnetic metal (x = 1, i.e., CaCrO3) phase transitions. Cr changes its oxidation state from 3+ in LaCrO3 to 4+ in CaCrO3, showing both 3+ and 4+ states for intermediate compositions. Interestingly, the introduction of Hubbard energy U and Ca substitution affects Cr–O hybridization, as observed in partial density of states. A compositional phase diagram with magnetic ground state is presented for the La1−xCaxCrO3 (0 ≤ x ≤ 1) system.
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