Experimental Physics V, Center for Electronic Correlations and Magnetism, University of Augsburg, Augsburg, Germany.
J Phys Condens Matter. 2013 Mar 27;25(12):126002. doi: 10.1088/0953-8984/25/12/126002. Epub 2013 Feb 28.
La2RuO5 shows a magneto-structural phase transition at 161 K with spin dimerization and concomitant formation of a non-magnetic singlet ground state. To gain a deeper insight into the origin of this transition systematic substitution of Ru by Ti has been carried out. Polycrystalline samples have been synthesized by thermal decomposition of citrate precursors leading to La2Ru(1-y)Ti(y)O5 (0 ≤ y ≤ 0.45). The crystal structure was investigated by x-ray powder diffraction at room temperature and at 100 K. The valences of Ti and Ru were obtained from x-ray absorption near edge structure spectroscopy at the Ti-K and the Ru-LIII absorption edges, respectively. The magnetic phase transition was investigated by magnetic susceptibility measurements as a function of Ti substitution, revealing a decreasing transition temperature on increasing the level of substitution. The step-like feature in the magnetic susceptibility reflecting the Ru-Ru spin dimerization transition becomes smeared out close to y = 0.3 and completely vanishes at y = 0.45, indicating complete suppression of spin-dimer formation. Additional specific-heat measurements show a continuous decrease of the magnetic entropy peak with increasing Ti substitution mirroring the reduced number of spin dimers due to the magnetic dilution. A magnetic anomaly of the dimerization transition can hardly be detected for y ≥ 0.3. Density functional theory calculations were carried out to study changes of the electronic band structure caused by the substitution. A possibly preferred distribution of Ti and Ru and the magnetic interactions as well as the change of the density of states close to the Fermi level are investigated. Based on these experimental results a detailed (y,T) phase diagram is proposed.
La2RuO5 在 161 K 时表现出磁结构相变,自旋二聚化并伴随形成非磁性单重态基态。为了更深入地了解这种转变的起源,系统地用 Ti 取代 Ru 已经进行了研究。通过热分解柠檬酸前体制备了多晶样品,得到了 La2Ru(1-y)Ti(y)O5(0 ≤ y ≤ 0.45)。室温及 100 K 下采用 X 射线粉末衍射研究了晶体结构。Ti-K 和 Ru-LIII 吸收边的 X 射线吸收近边结构光谱分别获得了 Ti 和 Ru 的价态。通过磁导率测量研究了磁相变随 Ti 取代的变化,发现随着取代水平的增加,转变温度降低。在磁导率中反映 Ru-Ru 自旋二聚化转变的阶跃特征变得模糊,在 y = 0.3 附近完全消失,表明自旋二聚体的完全抑制。附加的比热测量表明,随着 Ti 取代的增加,磁熵峰连续减小,反映出由于磁稀释导致的自旋二聚体数量减少。对于 y ≥ 0.3,几乎无法检测到二聚化转变的磁异常。进行了密度泛函理论计算,以研究取代引起的电子能带结构的变化。研究了 Ti 和 Ru 的可能优先分布、磁相互作用以及费米能级附近态密度的变化。基于这些实验结果,提出了详细的(y,T)相图。