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JOURNALS // Fizika Tverdogo Tela // Archive

Fizika Tverdogo Tela, 2012 Volume 54, Issue 4, Pages 730–733 (Mi ftt12827)

This article is cited in 3 papers

Magnetism

X-ray emission studies of evolution of the electron and spin structures of Mn in mixed manganites Ln$_{1-x}$Sr$_x$MnO$_3$ (Ln = La, Sm, and Ce)

A. E. Sovestnova, B. T. Melekhb, V. V. Fedorovac, È. V. Fomina

a The Petersburg Nuclear Physics Institute, The National Research Center "Kurchatov Institute"
b Ioffe Institute, St. Petersburg
c Peter the Great St. Petersburg Polytechnic University

Abstract: The chemical shift $\Delta E_{K\beta1}$ and the exchange splitting $\Delta E_{\mathrm{split}}$ of the emission X-ray Mn $K_{\beta1}$ line in mixed manganites Ln$_{1-x}$Sr$_x$MnO$_3$ (Ln = La, Sm, and Ce) have been systematically studied for the first time. It has been found that $\Delta E_{K\beta1}$ and $\Delta E_{\mathrm{split}}$ are almost the same in the range $x <$ 0.4–0.5, as is the case in Mn$_2$O$_3$, and then they decrease relatively quickly to the values characteristic of MnO$_2$. It has been assumed that such a behavior corresponds to the model where in the region of hole doping ($x <$ 0.5), the ground state is a mixture of configurations Mn$^{3+}$ 3$d^4$ and 3$d^4\underline{L}$, so that the second configuration fraction increases with $x$. At high values of $x$, the configuration Mn$^{4+}$ 3$d^3$ should be taken into account; the contribution of this configuration increases with increasing degree of doping, and it becomes dominant at $x$ = 1. In all cases, the manganese state is high-spin.

Received: 19.07.2011
Accepted: 30.09.2011


 English version:
Physics of the Solid State, 2012, 54:4, 778–781

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