首页> 外文会议>Symposium on Science and Technology of Magnetic Oxides December 1-4, 1997, Boston, Massachusetts, U.S.A. >The local atomic structure of La_(1-x)Sr_xCoO_3: effects induced by the spin-state and non-metal to metal transitions
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The local atomic structure of La_(1-x)Sr_xCoO_3: effects induced by the spin-state and non-metal to metal transitions

机译:La_(1-x)Sr_xCoO_3的局部原子结构:自旋态和非金属到金属跃迁引起的效应

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The pair density function (PDF) used in the analysis of pulsed neutron diffraction data of La_(1-x)Sr_xCoO_3 revealed new structural effects which are correlated to the susceptibility and transport transitions. The transition in the spin configuration of the Co ions frm the low-spin (LS) to the high-spin (HS) state in the Co perovskite oxides can potentially induce structural distortions due to the coupling of the spin to the lattice and charge. The ground state of the pure compound, LaCo_3, is in the LS state and is non-magnetic. A transition occurs to the HS state at approx 50 K as indicated from the susceptibility measurements due to the thermal excitation of electrons to the e_g level. The Co_(LS)O_6 octahedra associated with the Co ions in the LS configuration are distinguished from the Co_(HS)O_6 octahedra with the Co in the HS coonfiguration because the CO_(LS)-O bound length is shorter than the Co_(HS)-O distance due to the different size of the corresponding Co ions. Such bond lenths are clearly identified in the local structure between 15-300 K. This finding is in contrast to the average structure which lshws only one type of bond length in this temperature range but two types of bond lengths are suggested at considerably higher temperatures. This suggests that whereas the LS and HS CoO_4-octahedra coexist, they are randomly distributed in the crystal lattice at lower temperatures and become ordered at higher temperatures. The introduction of charge carriers in the structure does not eliminate the coexistence of both the LS and HS states, indicating that with the transition to the ferromagnetic metallic state, the spin configuration is not entirely of the HS character and structural inhom,ogeneities are present.
机译:La_(1-x)Sr_xCoO_3的脉冲中子衍射数据分析中使用的对密度函数(PDF)揭示了与磁化率和迁移跃迁相关的新结构效应。钙钛矿型钴氧化物中从低自旋(LS)态到高自旋(HS)态的Co离子自旋构型的转变可能会由于自旋与晶格和电荷的耦合而潜在地引起结构变形。纯化合物LaCo_3的基态处于LS状态,并且是非磁性的。如从磁化率测量所表明的,由于电子热激发到e_g能级,在大约50 K处发生了向HS状态的跃迁。 LS配置中与Co离子关联的Co_(LS)O_6八面体与HS配比中的Co不同于Co_(HS)O_6八面体,因为CO_(LS)-O的结合长度短于Co_(HS )-O距离是由于相应Co离子的尺寸不同所致。可以在15-300 K之间的局部结构中清楚地识别出这样的键长度。这一发现与平均结构相反,该平均结构在该温度范围内仅显示一种键长,但是在更高的温度下建议使用两种键长。这表明,虽然LS和HS CoO_4-八面体共存,但它们在较低温度下随机分布在晶格中,并在较高温度下变得有序。在结构中引入电荷载流子并不能消除LS和HS状态的共存,这表明随着向铁磁金属态的转变,自旋构型不完全具有HS特性,并且存在结构不均一性。

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