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Phys. Rev. B 80, 125112 (2009) [8 pages]

Role of K/Bi disorder in the electronic structure of β-K2Bi8Se13

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Khang Hoang1, Aleksandra Tomic2, S. D. Mahanti2,*, Theodora Kyratsi3, Duck-Young Chung4, S. H. Tessmer2, and Mercouri G. Kanatzidis4,5
1Materials Department, University of California, Santa Barbara, California 93106, USA
2Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
3Department of Mechanical and Manufacturing Engineering, University of Cyprus, Nicosia 1678, Cyprus
4Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
5Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA

Received 30 March 2009; revised 29 June 2009; published 15 September 2009

We have carried out tunneling spectroscopy and first-principles studies for β-K2Bi8Se13, a promising thermoelectric material with partially disordered mixed K/Bi sites. The tunneling data, obtained with a scanning tunneling microscope (STM), show that the system is a semiconductor with a band gap of ∼0.4 eV and band-tail states near the valence-band top and the conduction-band bottom. First-principles calculations, on the other hand, show that β-K2Bi8Se13 can be semimetallic or semiconducting depending on the arrangements of the K and Bi atoms in the mixed sites. The electronic structure of β-K2Bi8Se13 near the band-gap region is largely determined by unbonded Se p states and states associated with strained bonds which are present due to K/Bi disorder and by the Bi p-Se p hybridization which tends to drive the system toward metallicity. Among the different K/Bi arrangements investigated, we have identified a structural model (quasidisordered structure) that is able to satisfactorily reproduce the atomic and electronic structures of β-K2Bi8Se13; i.e., the local composition in the mixed channels as observed experimentally and the band gap and tails as seen in the STM measurements. We argue that transport properties of β-K2Bi8Se13 can be qualitatively understood in terms of the electronic structure obtained in calculations using the above structural model.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.80.125112
DOI:
10.1103/PhysRevB.80.125112
PACS:
71.20.Nr, 71.23.An, 72.15.Jf

*Corresponding author; mahanti@pa.msu.edu