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Charge-Density-Wave Order and Multiple Magnetic Transitions in Divalent Europium Compound EuAl4
Journal of the Physical Society of Japan ( IF 1.7 ) Pub Date : 2021-05-17 , DOI: 10.7566/jpsj.90.064704
Koji Kaneko 1, 2 , Takuro Kawasaki 2 , Ai Nakamura 3, 4 , Koji Munakata 5 , Akiko Nakao 5 , Takayasu Hanashima 5 , Ryoji Kiyanagi 2 , Takashi Ohhara 2 , Masato Hedo 6 , Takao Nakama 6 , Yoshichika Ōnuki 6, 7
Affiliation  

Multiple transition phenomena in divalent Eu compound EuAl4 with the tetragonal structure were investigated via the single-crystal time-of-flight neutron Laue technique. At 30.0 K below a charge-density-wave (CDW) transition temperature of TCDW = 140 K, superlattice peaks emerge near nuclear Bragg peaks described by an ordering vector \(\boldsymbol{q}_{\text{CDW}} = (0,0,\delta _{c})\) with δc ∼ 0.19. In contrast, magnetic peaks appear at \(\boldsymbol{q}_{2} = (\delta _{2},\delta _{2},0)\) with δ2 = 0.085 in a magnetic-ordered phase at 13.5 K below TN1 = 15.4 K. By further cooling to below TN3 = 12.2 K, the magnetic ordering vector changes into \(\boldsymbol{q}_{1} = (\delta _{1},0,0)\) with δ1 = 0.17 at 11.5 K and slightly shifts to δ1 = 0.194 at 4.3 K. No distinct change in the magnetic Bragg peak was detected at TN2 = 13.2 K and TN4 = 10.0 K. The structural modulation below TCDW with qCDW is characterized by the absence of the superlattice peak in the (0 0 l) axis. As a similar CDW transition was observed in SrAl4, the structural modulation with qCDW could be mainly ascribed to the displacement of Al ions within the tetragonal ab-plane. Complex magnetic transitions are in stark contrast to a simple collinear magnetic structure in isovalent EuGa4. This could stem from different electronic structures with the CDW transition between two compounds.

中文翻译:

二价Euro化合物EuAl4中的电荷密度波阶和多重磁跃迁

通过单晶飞行时间中子Laue技术研究了具有四方结构的二价Eu化合物EuAl 4的多重跃迁现象。在T CDW = 140 K的电荷密度波(CDW)转变温度以下30.0 K处,超晶格峰出现在有序矢量描述的核布拉格峰附近\(\ boldsymbol {q} _ {\ text {CDW}} =(0,0,\ delta _ {c})\)δ Ç〜0.19。相反,磁峰出现在\(\ boldsymbol {q} _ {2} =(\ delta _ {2},\ delta _ {2},0)\)δ 2在磁性有序相= 0.085在低于13.5ķ Ť N1 = 15.4 K.通过进一步冷却至低于Ť N3 = 12.2 K,所述磁有序向量变为\(\ boldsymbol {q} _ {1} =(\ delta _ {1},0,0)\)δ 1 = 0.17 11.5 K和略微移向δ 1 = 0.194 4.3在磁布拉格峰K.没有明显的变化,在检测到Ť N2 = 13.2 K和Ť N4 = 10.0 K.下面的结构调制Ť CDWq CDW的特征是在(0 0 l)轴上不存在超晶格峰。由于在SrAl 4中观察到了类似的CDW跃迁,因此q CDW的结构调节可能主要归因于四方晶胞内Al离子的位移。-飞机。复杂的磁跃迁与等价EuGa 4中的简单共线磁结构形成鲜明对比。这可能源于两种化合物之间CDW跃迁的不同电子结构。
更新日期:2021-05-17
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