Mn K-edge XANES studies of the La(1-x) A(x) MnO(3) systems (A = Ca, Ba, Pb)
Mn K-edge XANES studies of the La(1-x) A(x) MnO(3) systems (A = Ca, Ba, Pb)
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La(1-x) A(x) MnO(3) 体系（A = Ca、Ba、Pb）的 Mn K 边 XANES 研究
DOI：
10.1103/physrevb.63.214405
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发表时间：
2001
影响因子：
3.7
通讯作者：
E. Brosha
中科院分区：
文献类型：
--
作者：
F. Bridges;C. Booth;Mark Anderson;G. Kwei;J. Neumeier;J. Snyder;J. Mitchell;J. Gardner;E. Brosha
We present Mn K-edge x-ray absorption near-edge structure (XANES) data for a number of manganite systems as a function of temperature. The $1s$ absorption edge for the Ca-substituted samples is very sharp, almost featureless, and shifts uniformly upwards with increasing Ca content. The interpretation of this result is controversial because the lack of structure appears difficult to reconcile with a mixture of ${\mathrm{Mn}}^{+3}$ and ${\mathrm{Mn}}^{+4}$ ions or with several different Mn-O bond lengths at high T. We propose a possible solution in terms of covalency and considerable overlap of the Mn p states (mostly Mn $4p).$ The manganite preedge structure is quite similar to that for a large number of other Mn compounds, with two or three small peaks that are ascribed to $1s\ensuremath{-}3d$ weakly allowed dipole transitions plus possibly a small quadrupole component. The weak dipole transitions are explained as arising from a hybridization of the Mn $4p$ state of the excited atom with an odd symmetry combination of Mn $3d$ states on adjacent Mn atoms. The first preedge peak ${\mathrm{A}}_{1}$ has a small shift to higher energy with increasing valence while the next peak ${\mathrm{A}}_{2}$ is nearly independent of dopant concentration at 300 K. However, for the colossal magnetoresistance (CMR) samples the ${\mathrm{A}}_{2}$ preedge peak shifts to a lower energy below the ferromagnetic transition temperature ${T}_{c},$ resulting in a decrease in the ${\mathrm{A}}_{2}\ensuremath{-}{\mathrm{A}}_{1}$ splitting by $\ensuremath{\sim}0.4 \mathrm{eV}.$ This indicates a change in the higher-energy $3d$ bands, most likely the minority spin ${e}_{g},$ plus some change in covalency. In addition, the amplitudes are temperature dependent for the CMR materials, with the change in ${\mathrm{A}}_{1},$ ${\mathrm{A}}_{2}$ correlated with the change in sample magnetization. For the charge ordered (CO) sample, the analysis suggests that the change in the preedge is produced by a distortion that increases below ${T}_{\mathrm{CO}}.$ We discuss these results in terms of some of the theoretical models that have been proposed and other recent XANES studies.
We present Mn K-edge x-ray absorption near-edge structure (XANES) data for a number of manganite systems as a function of temperature. The $1s$ absorption edge for the Ca-substituted samples is very sharp, almost featureless, and shifts uniformly upwards with increasing Ca content. The interpretation of this result is controversial because the lack of structure appears difficult to reconcile with a mixture of ${\mathrm{Mn}}^{+3}$ and ${\mathrm{Mn}}^{+4}$ ions or with several different Mn-O bond lengths at high T. We propose a possible solution in terms of covalency and considerable overlap of the Mn p states (mostly Mn $4p).$ The manganite preedge structure is quite similar to that for a large number of other Mn compounds, with two or three small peaks that are ascribed to $1s\ensuremath{-}3d$ weakly allowed dipole transitions plus possibly a small quadrupole component. The weak dipole transitions are explained as arising from a hybridization of the Mn $4p$ state of the excited atom with an odd symmetry combination of Mn $3d$ states on adjacent Mn atoms. The first preedge peak ${\mathrm{A}}_{1}$ has a small shift to higher energy with increasing valence while the next peak ${\mathrm{A}}_{2}$ is nearly independent of dopant concentration at 300 K. However, for the colossal magnetoresistance (CMR) samples the ${\mathrm{A}}_{2}$ preedge peak shifts to a lower energy below the ferromagnetic transition temperature ${T}_{c},$ resulting in a decrease in the ${\mathrm{A}}_{2}\ensuremath{-}{\mathrm{A}}_{1}$ splitting by $\ensuremath{\sim}0.4 \mathrm{eV}.$ This indicates a change in the higher-energy $3d$ bands, most likely the minority spin ${e}_{g},$ plus some change in covalency. In addition, the amplitudes are temperature dependent for the CMR materials, with the change in ${\mathrm{A}}_{1},$ ${\mathrm{A}}_{2}$ correlated with the change in sample magnetization. For the charge ordered (CO) sample, the analysis suggests that the change in the preedge is produced by a distortion that increases below ${T}_{\mathrm{CO}}.$ We discuss these results in terms of some of the theoretical models that have been proposed and other recent XANES studies.