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Phys. Rev. B 68, 085102 (2003) [11 pages]

Experimental and theoretical investigation of optical properties of dysprosium monopnictides

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J. Schoenes
Institut für Halbleiterphysik und Optik, Technische Universität Braunschweig, D-38106 Braunschweig, Germany

P. Repond and F. Hulliger
Laboratorium für Festkörperphysik, ETH Zürich, CH-8093 Zürich, Switzerland

D. B. Ghosh and S. K. De
Department of Materials Science, Indian Association for the Cultivation of Science, Jadavpur, Calcutta 700 032, India

J. Kuneš
Institute of Physics, Academy of Sciences, Cukrovarnická 10, CZ-162 53 Prague, Czech Republic

P. M. Oppeneer
Leibniz-Institute of Solid State and Materials Research, P.O. Box 270016, D-01171 Dresden, Germany

Received 3 March 2003; published 5 August 2003

The electronic and optical properties of DyP and DyBi are investigated both experimentally and computationally. The reflectivity spectra, which have been measured up to 12 eV on single crystals, display richly peaked spectral structures that are analogous for both pnictides. From the measured reflectivities the plasma frequencies, Drude relaxation times, and optical conductivity spectra are derived. The fitted Drude conductivity reveals that DyP and DyBi are semimetals with a number of free carriers of about 0.16 and 0.23 per formula unit, respectively. The very-structured experimental optical conductivity spectra are compared to calculated spectra, which are computed using two different approaches to the Dy 4f states: the open-core approach and the L(S)DA+U approach in three versions. These approaches to the 4f states lead to very similar optical spectra. There exists a reasonable agreement between calculation and experiment for a number of the spectral features, which are interpreted by specific interband transitions within the calculated band structure. The agreement between theory and experiment substantiates that the 4f electrons do not participate in the bonding. The differences that remain between theory and experiment for some of the spectral features do not appear to rest on aspects of the treatment of the 4f states, but rather to be intrinsic shortcomings in the description of the other band states.

© 2003 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.68.085102
DOI:
10.1103/PhysRevB.68.085102
PACS:
78.20.-e, 71.20.-b, 71.28.+d