带电有序Pr0.75Na0.25MnO3锰矿中Ni和Cr取代铁磁金属相的还原和Griffiths相的出现

Rozilah Rajmi
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摘要

Pr0.75Na0.25Mn1-xAxO3 (A = Ni, Cr)多晶样品X = 0, 0.03),并对其结构和磁性能进行了研究。单价掺杂的Pr0.75Na0.25MnO3表现出绝缘行为,这与电荷有序(CO)的存在导致载流子的强局域化有关。在CO Pr0.75Na0.25Mn1-xAxO3锰矿中,不同类型的磁性离子A (Ni2+和Cr3+)以x = 0.03的浓度取代Mn位,可以显著改变其结构和磁性能。x射线衍射图显示,所有样品均为单相,结晶为具有Pnma空间群的正交结构。Rietveld细化分析表明,Ni2+的取代使晶胞体积增大,而Cr3+的取代使晶胞体积减小,这可能是由于两种离子的离子半径不同所致。在ni -取代和cr -取代的样品中,CO态的抑制和铁磁金属态的诱导可能是由于分别诱导了Ni2+ -O-Mn4 +和Mn3+ -O-Cr3 +的双交换相互作用。ni取代和cr取代样品的磁性能变化可能是由于Ni2+ -O-Mn4 +和Mn3+ -O-Cr3 +之间存在不同强度的铁磁相互作用。此外,磁化率反曲线的温度依赖性与居里-魏斯定律的偏差表明,两种替代样品都存在Griffith类相行为。由于TC和TG值(TC-TG)的差异较大,ni取代的样品比cr取代的样品产生更大的GP效应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Revival of Ferromagnetic-Metallic Phase and Emergence of Griffiths Phase via Ni and Cr Substitution in Charged-Ordered Pr0.75Na0.25MnO3 Manganite
Polycrystalline samples of Pr0.75Na0.25Mn1-xAxO3 (A = Ni, Cr; x = 0, 0.03) were prepared using conventional solid-state method and their structural and magnetic properties were investigated. Monovalent-doped Pr0.75Na0.25MnO3 exhibits insulating behavior which is related to the strong localization of charge carriers due to the presence of charge ordering (CO). The substitution of different types of magnetic ions, A, which are Ni2+ and Cr3+, at a concentration of x = 0.03 at the Mn site in the CO Pr0.75Na0.25Mn1-xAxO3 manganite, has been found to dramatically modify its structural and magnetic properties. X-ray diffraction patterns showed that all samples were present in single phase and crystallized in orthorhombic structure with Pnma space group. The Rietveld refinement analysis showed that the unit cell volume increased due to Ni2+ substitution, while it decreased due to Cr3+ substitution, which may be attributed to the different ionic radii of both ions. The suppression of the CO state and the induction of the ferromagnetic-metallic state in the Ni-substituted and Cr-substituted samples are suggested to be due to the induction of double-exchange interaction involving Ni2+–O–Mn4+ and Mn3+–O–Cr3+, respectively. The variation in magnetic properties between the Ni-substituted and Cr-substituted samples is suggested to be due to the existence of different strengths of ferromagnetic interaction between Ni2+–O–Mn4+ and Mn3+–O–Cr3+. In addition, the deviation of the temperature dependence of the inverse magnetic susceptibility curves from the Curie-Weiss law suggests the existence of Griffith’s phase-like behaviour for both substitution samples. The Ni-substituted sample induced a greater GP effect than the Cr-substituted sample due to the larger difference of TC and TG value (TC-TG).
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