Hole distribution between the Ni 3d and O 2p orbitals in Nd2−xSrxNiO4−δ

Hu, Z. ; Golden, M. S. ; Fink, J. ; Kaindl, G. ; Warda, S. A. ; Reinen, D. ; Mahadevan, Priya ; Sarma, D. D. (2000) Hole distribution between the Ni 3d and O 2p orbitals in Nd2−xSrxNiO4−δ Physical Review B: Condensed Matter and Materials Physics, 61 (5). pp. 3739-3744. ISSN 1098-0121

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Official URL: http://prb.aps.org/abstract/PRB/v61/i5/p3739_1

Related URL: http://dx.doi.org/10.1103/PhysRevB.61.3739

Abstract

We present a joint experimental and theoretical study of x-ray absorption at the O-K and Ni-L2,3 thresholds of Nd2−xSrxNiO4−δ providing an analysis of the distribution of doped holes induced by Sr substitution between Ni 3d and O 2p orbitals. The preedge peak in the O-K x-ray absorption (XAS) spectra, reflecting holes located in the O 2p orbitals, increases monotonically with the degree of Sr doping up to the maximum doping level studied (x=1.4). The saturation in the relative intensity of the O-K preedge peak in the analogous lanthanum nickelate reported in the literature is shown to be most likely due to surface oxygen deficiency. Furthermore, the experimental Ni-L2,3 XAS spectrum of the Ni(III) nickelate Nd1.1Sr0.9NiO3.95 was simulated by a cluster approach, including charge-transfer and complete multiplet interactions, and compared with the corresponding spectrum of the Ni(III) system Nd2Li0.5Ni0.5O4. The 3d7 weight in the ground state of Nd1.1Sr0.9NiO3.95 was found to be 42%, somewhat smaller than the value of 51% found for Nd2Li0.5Ni0.5O4. This indicates the influence of nonlocal effects in x-ray-absorption spectroscopy, which, in this case is due to the increased covalency in the Sr-doped system as a result of inter-NiO6-cluster interaction. Such interactions are absent in Nd2Li0.5Ni0.5O4, which is characterized by having isolated NiO6 clusters.

Item Type:Article
Source:Copyright of this article belongs to The American Physical Society.
ID Code:46332
Deposited On:04 Jul 2011 06:54
Last Modified:18 May 2016 02:15

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