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Phase transitions in molecule-based magnets: Neutron diffraction, magnetic and specific heat studies.

机译:基于分子的磁体中的相变:中子衍射,磁性和比热研究。

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The crystallographic and magnetic properties for the M[N(CN) 2]2 (M = Mn, Fe, Co, Ni) series have been investigated by neutron diffraction, dc magnetization, ac susceptibility and specific heat on polycrystalline samples. The crystal structures for all compounds are isomorphous in the paramagnetic regime as well as in the ordered state, and consist of discrete octahedra which are axially elongated and successively tilted in the ab-plane. The zero-field magnetic structure for the Mn and Fe compounds consists of two sublattices which are antiferromagnetically coupled and spontaneously canted, with spin orientation mainly along the a-axis. There is a small uncompensated moment along the b-axis (Mn) and the c-axis (Fe). The zero-field magnetic structure for the Co and Ni compounds is collinear ferromagnetic with spin orientation along the c-axis. The results provide the first determination of a complete magnetic structure in the ordered state for a molecule-based magnet. The ground states are characterized by large magnetic anisotropy. The application of a magnetic field induces a spin rotation transition in the Mn compound and an energy-level crossing in the Fe compound. The do magnetization and in-field specific heat studies for Cu[N(CN) 2]2 reveal the previously unknown ferromagnetic ordering at low temperatures. Comparisons of the magnetic structures for the isostructural M[N(CN)2]2 (M = Mn, Fe, Co, Ni) series suggest that the spin direction is stabilized by crystal fields and the spin canting is induced by the successive tilting of the octahedra. We propose that the superexchange interaction is the mechanism responsible for the magnetic ordering in these compounds and we find that a crossover from noncollinear antiferromagnetism to collinear ferromagnetism occurs for a superexchange angle of αc = 142.0(5)°.
机译: M [N(CN) 2 ] 2 M = Mn,Fe的晶体学和磁学性质,Co,Ni)系列已通过中子衍射,直流磁化,磁化率和比热在多晶样品上进行了研究。所有化合物的晶体结构在顺磁态和有序态都是同构的,并且由离散的八面体组成,八面体轴向伸长并在 ab 平面中依次倾斜。 Mn和Fe化合物的零场磁结构由两个反铁磁耦​​合且自发倾斜的子晶格组成,其自旋方向主要沿 a 轴。沿 b 轴(Mn)和 c 轴(Fe)有一个小的未补偿力矩。 Co和Ni化合物的零磁场结构是共线铁磁,其自旋方向沿 c 轴。该结果为基于分子的磁体在有序状态下完整磁性结构的首次确定提供了条件。基态的特征在于大的磁各向异性。磁场的施加在Mn化合物中引起自旋旋转转变,并在Fe化合物中引起能​​级交叉。 Cu [N(CN) 2 ] 2 的做磁化和场内比热研究揭示了低温下以前未知的铁磁有序。等斜结构M M [N(CN) 2 ] 2 M = Mn, Fe,Co,Ni)系列表明自旋方向由晶体场稳定,并且自旋倾斜是由八面体的连续倾斜引起的。我们认为超交换相互作用是这些化合物中磁有序的机制,我们发现,对于α c = 142.0(5)°。

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