Mn K-edge XANES studies of La(1-x)A(x)MnO(3) systems (A = Ca, Ba, Pb) - art. no. 214405

Citation
F. Bridges et al., Mn K-edge XANES studies of La(1-x)A(x)MnO(3) systems (A = Ca, Ba, Pb) - art. no. 214405, PHYS REV B, 6321(21), 2001, pp. 4405
Citations number
56
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
01631829 → ACNP
Volume
6321
Issue
21
Year of publication
2001
Database
ISI
SICI code
0163-1829(20010601)6321:21<4405:MKXSOL>2.0.ZU;2-N
Abstract
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 absorpti on edge for the Ca-substituted samples is very sharp, almost featureless, a nd shifts uniformly upwards with increasing Ca content. The interpretation of this result is controversial because the lack of structure appears diffi cult to reconcile with a mixture of Mn+3 and Mn+4 ions or with several diff erent 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). Th e manganite preedge structure is quite similar to that for a large number o f other Mn compounds, with two or three small peaks that are ascribed to 1s -3d weakly allowed dipole transitions plus possibly a small quadrupole comp onent. The weak dipole transitions are explained as arising from a hybridiz ation of the Mn 4p stale of the excited atom with an odd symmetry combinati on of Mn 3d states on adjacent Mn atoms. The first preedge peak A(1) has a small shift to higher energy with increasing valence while the next peak A( 2) is nearly independent of dopant concentration at 300 K. However, for the colossal magnetoresistance (CMR) samples the A(2) preedge peak shifts to a lower energy below the ferromagnetic transition temperature T-c, resulting in a decrease in the A(2)-A(1) splitting by similar to 0.4 eV. This indica tes 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 temper ature dependent for the CMR materials, with the change in A(1), A(2) correl ated with the change in sample magnetization. For the charge ordered (CO) s ample, the analysis suggests that the change in the preedge is produced by a distortion that increases below T-CO. We discuss these results in terms o f some of the theoretical models that have been proposed and other recent X ANES studies.