Hostname: page-component-78c5997874-fbnjt Total loading time: 0 Render date: 2024-11-19T04:03:02.555Z Has data issue: false hasContentIssue false
  • English
  • Français

Electronic Structures of Halogenated Polysilanes

Published online by Cambridge University Press:  10 February 2011

Hideshi Motoyama ,
Kyozaburo Takeda  and
Kenji Shiraishi
Hideshi Motoyama
Affiliation:
Department of Materials Science and Engineering, School of Science and Engineering, Waseda University, Shinjyuku, Tokyo 169, Japan
Kyozaburo Takeda
Affiliation:
Department of Materials Science and Engineering, School of Science and Engineering, Waseda University, Shinjyuku, Tokyo 169, Japan
Kenji Shiraishi
Affiliation:
NTT Basic Research Laboratories, Atsugi 243-01, Japan
Get access

Abstract

The electronic structures of halogenated polysilanes (PSi), whose side chains are replaced by halogen (X) atoms, have been theoretically investigated based on the firstprinciples calculations. It was found that non-bonding (n) electrons localizing at the X atom produce an important orbital mixing with the u valence electrons delocalized in the direction of the PSi skeleton (a-n mixing). This a-n mixing splits the top of the valence bands, and creates unoccupied states in the band gap. This valence-band-splitting effectively narrows the band gap to the visible range, and the unoccupied state in the band gap has the potential to be an electron acceptor. Moreover, we also investigated several replacement patterns as well as the kind of replaced halogen species (X=F, Cl, Br, I). The dispersion and energy position of the unoccupied state(s) can be artificially tuned by these chemical modifications. Thus, halogenation can change PSi into optelectronic polymers with visible photoluminescence.

Type
Research Article
Information
MRS Online Proceedings Library (OPL) , Volume 486: Symposium H – Materials & Devices for Silicon Based Optoelectronics , 1997 , 385
Copyright
Copyright © Materials Research Society 1998

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

[1] West, R., J. Orgno. Met. Chem., 300, 327 (1986).Google Scholar
[2] Miller, R. P., Michl, J., Chem. Rev., 89, 1359 (1989).Google Scholar
[3] Takeda, K., J. Phy. Soc. Jpn., suppl. B, 1 (1994).Google Scholar
[4] Yamabe, T., Tanaka, K., Teramae, H., and Fukui, K., Syn. Metals, 1, 321 (1979/1980).Google Scholar
[5] Yamaguchi, Y., Syn. Metals, 52, 51 (1992).Google Scholar
[6] Arawal, B. K. and Ghosh, B. K., J. Non-Cryst. Solids, 77 & 78, 1105 (1985).Google Scholar
[7] Fujino, M., Hisaki, T., Fujiki, M., and Matsumoto, N., Macromol., 25, 1079 (1992).Google Scholar
[8] Banovets, J. P., Suzuki, H., and Waymouth, R. M., Organometallics, 12, 4700 (1993).Google Scholar
[9] Stanislawski, D. A. and West, R., J. Organomet. Chem, 204, 307 (1981).Google Scholar
[10] Izydore, R. A. and McLean, S., J. Am. Chem. Soc, 97(19), 5612 (1975).Google Scholar
[11] Voronkov, M. G., Feshin, V. P., and Nikitin, P. A., J. Mol. Struct., 127, 181 (1985).Google Scholar
[12] In the present calculation, the x axis is in the direction of the PSi's main chain, and the xy plane is the skeleton plane.Google Scholar
[13] The level Mulliken charge localized at the side-chain halogen atom is calculated as follows; 40% for F, 78% for Cl, 81% for Br and 86% for I.Google Scholar