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Spin-Disorder and Non-Degenerate Energy States in Geometrically Frustrated Materials

机译:几何受挫材料中的自旋无序和非简并能态

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We have studied chalcogenide Ni$_{1-{rm x}}$Fe$_{rm x}$Ga$_{2}$ S$_{4}$ , showing geometrical frustration effect. M-H curves at 4.2 K reveal that the disordered spins cannot be rotated completely along the direction of high external field of 5 T, since these spins are strongly constrained in the triangular lattice. $H_{rm C}$ increases with increasing Fe concentration, being consistent with the enhanced antiferromagnetic (AFM) spin-spin interactions and the suppressed spin-fluctuation due to the increase in freezing temperature $T_{rm f}$. The specific heat $(C_{rm p}/T)$ measurement do not show any phase transformation between 2 and 160 K and there is no clear indication of gap in the temperature dependent $C_{rm p}$ curve between 0 and 7 T, because the atomic short-range ordering of the strained spin in the geometrically frustrated triangular lattice exists at low temperature. Though typical geometrically frustrated magnet shows degeneracy, Mössbauer analysis at 4.2 K shows that 5D of 3d orbit in the samples studied here is splitted into ${}^{5}T_{2{rm g}}$ and ${}^{5}E_{2{rm g}}$, and ${}^{5}T_{2{rm g}}$ is further splitted into singlet and doublet by large electric quadrupole splitting. This suggests that Fe $^{2+}$ ionic state has no absolute degenerate energy states in all samples due to Jahn-Teller effect.
机译:我们研究了硫属元素化物Ni $ _ {1- {rm x}} $ Fe $ _ {rmrm} $ Ga $ _ {2} $ S $ _ {4} $,显示出几何挫折效应。在4.2 K时的M-H曲线表明,无序自旋不能完全沿着5 T的高外场方向旋转,因为这些自旋强烈地约束在三角形晶格中。 $ H_ {rm C} $随着Fe浓度的增加而增加,这与增强的反铁磁(AFM)自旋-自旋相互作用和由于冻结温度$ T_ {rm f} $的升高而抑制的自旋波动相一致。比热$(C_ {rm p} / T)$的测量值在2至160 K之间未显示任何相变,也没有明确表明温度相关的$ C_ {rm p} $曲线在0至7之间存在间隙。 T,因为在低温下存在几何受挫的三角晶格中应变自旋的原子短程排序。尽管典型的几何受挫磁体显示出简并性,但在4.2 K的Mössbauer分析显示,此处研究的样本中3d轨道的5D分为$ {} ^ {5} T_ {2 {rm g}} $和$ {} ^ {5 } E_ {2 {rm g}} $和$ {} ^ {5} T_ {2 {rm g}} $通过大四极电子分裂进一步分裂为单峰和双峰。这表明由于Jahn-Teller效应,Fe $ ^ {2 +} $离子态在所有样品中都没有绝对简并的能量态。

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