论文标题
Collinear抗铁磁序列中的旋转 - $ \ frac52 $三角晶格抗fiferromagnet na $ _3 $ _3 $ fe(po $ _4 $)$ _ 2 $
Collinear antiferromagnetic order in spin-$\frac52$ triangle lattice antiferromagnet Na$_3$Fe(PO$_4$)$_2$
论文作者
论文摘要
我们提出了沮丧的旋转的结构和磁性-5/2 $三角形晶格抗fiferromagnet na $ _3 $ _3 $ fe(po $ _4 $)$ _ 2 $通过X射线衍射,磁化,热量,热容量和中子衍射测量值对多晶样品进行了衍射测量。除了系统的晶格收缩外,从依赖温度依赖的X射线衍射从温度依赖性X射线衍射中检测到结构性失真。高温下的磁敏感性与高温系列的扩展非常吻合 - $ 5/2 $同型三角晶格抗fiferromagnet,平均交换耦合为$ j/k _ {\ rm b} \ simeq 1.8 $ k,而不是单级$ 5/2 $ 5/2 $ 5/2 $ 2 $ 2 $ 2 $ 2 $ 5/2 $ 5/脉冲场磁化数据的饱和场一致地重现了交换耦合的该值。它在$ t _ {\ rm n} \ simeq 10.4 $ k中经历磁性长距离级。挫败率的中间值($ f \ simeq 3.6 $)反映了化合物中的适度挫败感,这通过减少有序的磁矩为$ \ sim 1.52 $ 1.52 $ $ $ _ {\ rm b} $在1.6 k时,与其经典价值相比($5μ_ _ _ {\ rm b} $)。磁等温线在$ h _ {\ rm sf} \ simeq3.2 $ t.磁场诱导的自旋流动过渡的变化中显示出变化。
We set forth the structural and magnetic properties of the frustrated spin-$5/2$ triangle lattice antiferromagnet Na$_3$Fe(PO$_4$)$_2$ examined via x-ray diffraction, magnetization, heat capacity, and neutron diffraction measurements on the polycrystalline sample. No structural distortion was detected from the temperature-dependant x-ray diffraction down to 12.5 K, except a systematic lattice contraction. The magnetic susceptibility at high temperatures agrees well with the high-temperature series expansion for a spin-$5/2$ isotropic triangular lattice antiferromagnet with an average exchange coupling of $J/k_{\rm B} \simeq 1.8$ K rather than a one-dimensional spin-$5/2$ chain model. This value of the exchange coupling is consistently reproduced by the saturation field of the pulse field magnetization data. It undergoes a magnetic long-range-order at $T_{\rm N} \simeq 10.4$ K. Neutron diffraction experiments elucidate a collinear antiferromagnetic ordering below $T_{\rm N}$ with the propagation vector $k = (1,0,0)$. An intermediate value of frustration ratio ($f \simeq 3.6$) reflects moderate frustration in the compound which is corroborated by a reduced ordered magnetic moment of $\sim 1.52$ $μ_{\rm B}$ at 1.6 K, compared to its classical value ($5 μ_{\rm B}$). Magnetic isotherms exhibit a change of slope envisaging a field induced spin-flop transition at $H_{\rm SF}\simeq3.2$ T. The magnetic field vs temperature phase diagram clearly unfold three distinct phase regimes, reminiscent of a frustrated magnet with in-plane (XY-type) anisotropy.