首页> 外文期刊>The European physical journal, B. Condensed matter physics >Interplay of structural, magnetic and transport properties in the layered Co-based perovskite LnBaCo_2O_5 (Ln = Tb, Dy, Ho)
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Interplay of structural, magnetic and transport properties in the layered Co-based perovskite LnBaCo_2O_5 (Ln = Tb, Dy, Ho)

机译:层状钴基钙钛矿LnBaCo_2O_5(Ln = Tb,Dy,Ho)中结构,磁性和输运性质的相互作用

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The oxygen deficient cobaltites LnBaCo_2O_5 (Ln = Tb, Dy, Ho) exhibit two successive crystallographic transitions at T_N ~ 340 K and at T_(CO) ~ 210 K. Whereas the first transition (P4/mmm to Pmmm) is related to the long-range antiferromagnetic ordering of the Co ions (spin ordering), the second transition (Pmmm to Pmmb) corresponds to the long-range ordering of the Co~(2+) and Co~(3+) species (charge ordering) occurring in 1:1 ratio in the structure. The charge ordered (CO) state was directly evidenced by the observation of additional superstructure peaks using neutron and electron diffraction techniques. The CO state was also confirmed indirectly from refinement of high resolution neutron diffraction data as well as from resistivity and DSC measurements. From the refined saturated magnetic moment values only, ~3.7μ_B and ~2.7μ_B, the electronic configuration of the Co ions in LnBaCo_2O_5 remains conjectural. Two pictures, with Co~(3+) ions either in intermediate spin state (t_(2g)~5e_g~1) or in high spin state (t_(2g)~4e_g~2), describe equally well our experimental data. In both cases, the observed magnetic structure can be explained using the qualitative Goodenough-Kanamori rules for superexchange. Finally, in contrast to the parent Ln = Y compound [Vogt et al., Phys. Rev. Lett. 84, 2969 (2000)], we do not report any spin transition in LnBaCo_2O_5 (Ln = Tb, Dy, Ho).
机译:缺氧钴矿LnBaCo_2O_5(Ln = Tb,Dy,Ho)在T_N〜340 K和T_(CO)〜210 K处表现出两个连续的晶体转变。离子的高范围反铁磁排序(自旋排序),第二个跃迁(Pmmm到Pmmb)对应于Co〜(2+)和Co〜(3+)物种的长距离排序(电荷排序)结构中的比例为1:1。通过使用中子和电子衍射技术观察其他超结构峰,直接证明了电荷有序(CO)状态。 CO态还通过高分辨率中子衍射数据的精炼以及电阻率和DSC测量间接证实。仅从精制的饱和磁矩值〜3.7μB和〜2.7μB,LnBaCo_2O_5中的Co离子的电子构型仍然是推测的。两幅图片,其中Co〜(3+)离子处于自旋态(t_(2g)〜5e_g〜1)或处于高自旋态(t_(2g)〜4e_g〜2),同样很好地描述了我们的实验数据。在这两种情况下,都可以使用超交换的定性Goodenough-Kanamori定律解释观察到的磁结构。最后,与母体Ln = Y化合物相反[Vogt等,Phys。牧师84,2969(2000)],我们没有报告LnBaCo_2O_5中有任何自旋跃迁(Ln = Tb,Dy,Ho)。

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