Determination of the orbital moment and crystal field splitting in LaTiO3

Utilizing a sum-rule in a spin-resolved photoelectron spectroscopic experiment with circularly polarized light, we show that the orbital moment in LaTiO$_3$ is strongly reduced both below and above the N\'{e}el temperature. Using Ti $L_{2,3}$ x-ray absorption spectroscopy as a local probe, we f...

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Bibliographic Details
Main Author: Haverkort, Maurits W. (Author)
Format: Article (Journal) Chapter/Article
Language:English
Published: 2004
In: Arxiv

Online Access:Verlag, kostenfrei, Volltext: http://arxiv.org/abs/astro-ph/0405516
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Author Notes:M.W. Haverkort, Z. Hu, A. Tanaka, G. Ghiringhelli, H. Roth, M. Cwik, T. Lorenz, C. Schuessler-Langeheine, S.V. Streltsov, A.S. Mylnikova, V.I. Anisimov, C. de Nadai, N.B. Brookes, H.H. Hsieh, H.-J. Lin, C.T. Chen, T. Mizokawa, Y. Taguchi, Y. Tokura, D.I. Khomskii, and L.H. Tjeng
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Summary:Utilizing a sum-rule in a spin-resolved photoelectron spectroscopic experiment with circularly polarized light, we show that the orbital moment in LaTiO$_3$ is strongly reduced both below and above the N\'{e}el temperature. Using Ti $L_{2,3}$ x-ray absorption spectroscopy as a local probe, we found that the crystal field splitting in the $t_{2g}$ subshell is about 0.12-0.30 eV. This large splitting does not facilitate the formation of an orbital liquid.
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