Hostname: page-component-5c6d5d7d68-vt8vv Total loading time: 0.001 Render date: 2024-08-22T22:20:27.888Z Has data issue: false hasContentIssue false

Oxygen Bonding in Bismuth Layered Compounds SrBi2Ta2O9

Published online by Cambridge University Press:  01 February 2011

Dong Su
Affiliation:
free_sd@hotmail.com, Arizona State Univ., Dept. of Physics, P.O. Box 871504, Tempe, AZ, 85287-1504, United States, 2174192783
Nan Jiang
Affiliation:
nan.jiang@asu.edu, Arizona State University, Department of physics, P.O. Box 871504, Tempe, AZ, 85287-1504, United States
Jianguo Wen
Affiliation:
jgwen@uiuc.edu, University of Illinois at Urbana-Champaign, Frederick Seitz Materials Research Laboratory, Urbana, IL, 61801, United States
Jianshe Liu
Affiliation:
jsliu@tsinghua.edu.cn, Tsinghua Unversity, Institute of Microelectronics, Beijing, 100084, China, People's Republic of
Get access

Abstract

With the help of the high resolution Z-contrast scanning transmission electron microscopy (STEM), the near edge fine structures of the electron loss spectroscopy (EELS) arises from different layers are investigated in SBT. The EELS spectra are interpreted by comparing with the calculation using linearnized augment plane wave (LAPW) method within the local density approximation (LDA). The oxygen bonding nature in different layers are discussed. In Bi2O2 layer, oxygen 2p state interacted with the Bi 6p state leads to a high t2g state in density of state while in SrTa2O7 layer, oxygen 2p state hybridized with Ta 5d and Sr 5d, which leads a higher eg state than t2g state.

Type
Research Article
Copyright
Copyright © Materials Research Society 2007

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Reference:

[1] Scott, J. F. and Araujo, C. A. Paz de, Science 246, 1400 (1989).Google Scholar
[2] Araujo, C. A-Paz de, Cuchiaro, J. D., McMillan, L. D., Scott, M. C., and Scott, J. F., (London)Nature(London) 374, 627 (1995).Google Scholar
[3] shimakawa, Y., Kubo, Y., Nakagawa, Y., Goto, S., Kamiyama, T., Asano, H., and Izumi, F., Phys. Rev. B 61, 6559(2000).Google Scholar
[4] Park, B. H., Hyun, S. J., Bu, S. D., Noh, T. W., Lee, J., Kim, H-D., and Jo, W., Appl. Phys. Lett. 74, 1907 (1999).Google Scholar
[5] Muller, D. A., Sorsch, T., Moccio, S., Baumann, F. H., Evans-lutterodt, K., and Timp, G., Nature(London) 399, 758(1999); J. C. H. Spence, Reports on Progess in Physics, 69 (3),725(2006).Google Scholar
[6] The program package WIEN2k allows to perform electronic structure calculations of solids using density functional theory (DFT). Detail information can be found at http://www.wien2k.at/index.html. The muffin-tin sphere radii is the radius of atom sphere in calculation, inside a linear combination of radial functions time spherical harmonics is used and outside the atomic sphere region, a plane wave explanation is used. The calculation result is independent with the parameters in a range in this case.Google Scholar
[7] Su, D., Zhu, J. S., Xu, Q. Y., and Wang, Y. N., J. Appl. Phys, 93, 4784(2003).Google Scholar
[8] Chen, J. G., Surface Science Reports 30, 1152 (1997).Google Scholar
[9] Robertson, J., Chen, C. W., Warren, W. L., and Gutleben, C. D., Appl. Phys. Lett. 69, 1704 (1996).Google Scholar