论文标题
Kitaev量子旋转液体候选na $ _2 $ $ _2 $ _2 $ teo $ _6 $的电子和磁相图
Electronic and magnetic phase diagrams of Kitaev quantum spin liquid candidate Na$_2$Co$_2$TeO$_6$
论文作者
论文摘要
据报道,3 $ d^7 $ co $^{2+} $ - 基于绝缘磁铁\ ncto {}在蜂窝晶状体上具有很强的Kitaev相互作用,因此被视为Kitaev量子量子旋转液体候选者。但是,由于存在其他类型的相互作用,因此发生了自发的远程磁性顺序。通过施加的磁场抑制了该顺序,从而导致一系列相位,并最终导致磁矩的饱和度。精确的相图,相位的性质以及野外诱导的相的可能性是Kitaev量子自旋液相,仍然是争论的问题。在这里,我们测量了一组广泛的物理特性,以构建完整的温度场相图在10 t时沿$ a $ a $ a $ a^*$ - 轴的磁场以及沿$ c $ 60 t的部分相图。我们使用磁化,特异性热,磁化效应,磁曲线,介电常数和电偏振探测相位,这是一种对称敏感的探针。通过这些测量值,我们确定所有先前不完整的相边界,并找到新的高场相边界。我们发现在几个相边界处的介电常数和中等磁缩合耦合中的强磁耦合。此外,我们使用磁场下的电偏振测量值检测到磁序的对称性。基于我们的分析,在任何阶段或之后都没有在零或有限磁场下进行电极化。
The 3$d^7$ Co$^{2+}$-based insulating magnet \NCTO{} has recently been reported to have strong Kitaev interactions on a honeycomb lattice, and is thus being considered as a Kitaev quantum spin liquid candidate. However, due to the existence of other types of interactions, a spontaneous long-range magnetic order occurs. This order is suppressed by applied magnetic fields leading to a succession of phases and ultimately saturation of the magnetic moments. The precise phase diagram, the nature of the phases, and the possibility that one of the field-induced phases is a Kitaev quantum spin liquid phase are still a matter of debate. Here we measured an extensive set of physical properties to build the complete temperature-field phase diagrams to magnetic saturation at 10 T for magnetic fields along the $a$- and $a^*$-axes, and a partial phase diagram up to 60 T along $c$. We probe the phases using magnetization, specific heat, magnetocaloric effect, magnetostriction, dielectric constant, and electric polarization, which is a symmetry-sensitive probe. With these measurements we identify all the previously incomplete phase boundaries and find new high-field phase boundaries. We find strong magnetoelectric coupling in the dielectric constant and moderate magnetostrictive coupling at several phase boundaries. Furthermore, we detect the symmetry of the magnetic order using electrical polarization measurements under magnetic fields. Based on our analysis, the absence of electric polarization under zero or finite magnetic field in any of the phases or after...