Structural details and magnetic order of La1-xSrxCoO3 (x≤0.3)

被引:324
作者
Caciuffo, R
Rinaldi, D
Barucca, G
Mira, J
Rivas, J
Señarís-Rodríguez, MA
Radaelli, PG
Fiorani, D
Goodenough, JB
机构
[1] Univ Ancona, Ist Nazl Fis Mat, I-60131 Ancona, Italy
[2] Univ Ancona, Dipartimento Sci Mat & Terra, I-60131 Ancona, Italy
[3] Univ Santiago, Dept Fis Aplicada, E-15706 Santiago, Spain
[4] Univ A Coruna, Dept Quim Fundamental & Ind, E-15071 La Coruna, Spain
[5] Rutherford Appleton Lab, ISIS Facil, Didcot OX11 0QX, Oxon, England
[6] CNR, Ist Chim Mat, I-00016 Monterotondo, Roma, Italy
[7] Univ Texas, Ctr Mat Sci & Engn, Austin, TX 78712 USA
来源
PHYSICAL REVIEW B | 1999年 / 59卷 / 02期
关键词
D O I
10.1103/PhysRevB.59.1068
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10 less than or equal to x less than or equal to 0.30) has been studied by neutron diffraction, high-resolution electron microscopy, and magnetic susceptibility measurements. The results give direct evidence for an inhomogeneous distribution of the Sr2+ ions and the segregation of the material into hole-rich ferromagnetic regions and a hole-poor semiconducting matrix at lower values of x. The holes introduced by Sr doping are attracted to the Sr2+ ions where they stabilize to lowest temperatures an intermediate-spin state at neighboring trivalent cobalt. The antibonding e electrons so stabilized increase the mean unit-cell volume and are delocalized over the cobalt atoms of the cluster where they couple the localized t(5) configurations ferromagnetically, Long-range ferromagnetic order between clusters is realized even for Sr doping as low as x = 0.10. The transition to a spin glass state is observed only for Sr concentrations smaller than 0.10. The volume of a hole-rich cluster grows in a magnetic field, and the origin of the large negative magnetoresistance observed near Te for 0.15 less than or equal to x less than or equal to 0.25 appears to be due to a growth of the clusters to a percolation threshold. For x = 0.30, the sigma* band of the intermediate-spin state below Te is at the threshold of a transition from itinerant to polaronic conduction add, above T-C, the system transforms smoothly to a cluster state. [S0163-1829(99)01002-4].
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页码:1068 / 1078
页数:11
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