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Formation of incommensurate long-range magnetic order in the Dzyaloshinskii-Moriya antiferromagnet Ba$_2$CuGe$_2$O$_7$ studied by neutron diffraction

机译:形成不相称的远程磁序   Dzyaloshinskii-moriya反铁磁Ba $ _ $ $ CuGe $ _ $ $ O $ _7 $由中子研究   衍射

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摘要

Neutron diffraction on a triple-axis spectrometer and a small-angle neutronscattering instrument is used to study the magnetic phase transition intetragonal Ba$_2$CuGe$_2$O$_7$ at zero magnetic field. In addition to theincommensurate cycloidal antiferromagnetic (AFM) long-range order, we establishthat weak incommensurate ferromagnetism (FM) also arises below the transitiontemperature $T_N$ identified by sharp Bragg peaks close to the $\Gamma$ point.The intensities of both the incommensurate AFM and FM Bragg peaks vanishabruptly at $T_N$ indicative of a weak first-order transition. Above $T_N$,evidence is presented that the magnetic intensity within the tetragonal $(a,b)$plane is distributed on a ring in momentum space whose radius is determined bythe incommensurate wavevector of the cycloidal order. We speculate that theassociated soft fluctuations are at the origin of the weak first-ordertransition in the spirit of a scenario proposed by Brazovskii.
机译:使用三轴光谱仪和小角度中子散射仪上的中子衍射研究零磁场下四方Ba $ _2 $ CuGe $ _2 $ O $ _7 $的磁相变。除了不等距的摆线反铁磁(AFM)远距离有序外,我们确定弱的不等距铁磁性(FM)还会在转变温度$ T_N $下方出现,该温度由接近$ \ Gamma $点的陡峭布拉格峰确定。 AFM和FM Bragg的峰值在$ T_N $处消失,表明一阶转换很弱。在$ T_N $以上,有证据表明四角形$(a,b)$平面内的磁强度分布在动量空间中的一个环上,该环的半径由摆线阶数的不相称波矢确定。我们推测,按照Brazovskii提出的方案的精神,相关的软波动是弱一阶跃迁的起源。

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