Hostname: page-component-586b7cd67f-rcrh6 Total loading time: 0 Render date: 2024-11-29T07:24:01.027Z Has data issue: false hasContentIssue false

Photoelastic Waveguides Formed by Interfacial Reactions on Semiconductor Heterostructures

Published online by Cambridge University Press:  21 February 2011

L. S. Yu
Affiliation:
University of California, San Diego, CA.
Z F. Guan
Affiliation:
University of California, San Diego, CA.
F. Deng
Affiliation:
University of California, San Diego, CA.
Q.Z. Liu
Affiliation:
University of California, San Diego, CA.
S. A. Pappert
Affiliation:
University of California, San Diego, CA.
P. K. L. Yu
Affiliation:
University of California, San Diego, CA.
S. S. Lau
Affiliation:
University of California, San Diego, CA.
J. Redwing
Affiliation:
University of Wisconsin, Madison, WI.
J. Geisz
Affiliation:
University of Wisconsin, Madison, WI.
T. F. Kuech
Affiliation:
University of Wisconsin, Madison, WI.
H. Kattelus
Affiliation:
Semiconductor Research Laboratory, VTT, Espoo, Finland.
I. Suni
Affiliation:
Semiconductor Research Laboratory, VTT, Espoo, Finland.
Get access

Abstract

Lateral confinement of carriers and photons in semiconductor heterostructures is an important feature in modern electronic and optoelectronic devices. A number of techniques have been invented to induce lateral confinement with varying degrees of success and processing requirements. One of simplest but least commonly used technique is to utilize the strain induced effect (or the photoelastic effect) to cause confinement. While the concept is simple, the control of stress in the stressor layers is rather difficult in practice, without resorting to complicated selective growth of strained layers. We have investigated the controlled introduction of stable stresses into semiconductor heterostructures using a simple scheme of interfacial reactions between a metal and the substrate. Since the volumetric change for a given reaction is fixed, the induced stress in the structure is independent of the deposition method or the deposition system, as long as the deposited film is fully reacted to form a compound. The stability of the stress depends on the stability of the compound. We have made low-loss (~ ldB/cm at 1.53 μm) photoelastic waveguides in GaAs/AlGaAs and other layered structures by reacting Ni and other metals, with an underlying semiconductor. In the case Ni on GaAs/AlGaAs, the dominant stressor compound is N3GaAs, and the waveguide characteristics are thermally stable up to 600°C. Other photoelastic optical devices are also demonstrated.

Type
Research Article
Copyright
Copyright © Materials Research Society 1994

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 For a review, see Deppe, D. and Holonyak, N., Jr.,J. Appl. Phys. 64, R93 (1988).Google Scholar
2 Xia, W., Pappert, S. A., Zhu, B., Clawson, A. R., Yu, P. K. L., Lau, S. S., Poker, D. B., White, C. W., and Schwarz, S. A., J. Appl. Phys. 71,2602 (1992).Google Scholar
3 Kirkby, P. A., Selway, P. R. and Westbrook, L. D., J. Appl. Phys., 50(7), 4567 (1979).Google Scholar
4 Yu, L. S., Guan, Z. F., Liu, Q. Z., Deng, F., Pappert, S. A., Yu, P. K. L., Lau, S. S., Florez, L. T. and Harbison, J. P., Appl. Phys. Lett. (1993).Google Scholar
5 Sands, T., Keramidas, V. G., Yu, A. J., Yu, K.-M., Gronsky, R., and Washburn, J., J. Mater. Res. 2(2), 262 (1987).Google Scholar
6 Kapon, E., Stoffel, N. G., Dobisz, E. A. and Bhat, R., Appl. Phys. Lett., 52(5), 351 (1988).Google Scholar
7 Lahav, A., Einzenberg, M., and Komen, Y., Mat. Res. Soc. Symp. Proc. 37, 641 (1985).Google Scholar
8 Sands, T., Keramidas, V. G., Yu, A. J., Yu, K-M., Gronsky, R., and Washbum, J., J. Mater. Res. 2 (2), 262 (1987).Google Scholar
9 Thornton, J. A. and Hoffman, D. W., J. Vac. Sci. Technol. 14,164 (1977).Google Scholar
10 Blachman, A. G., Metall. Trans. 2, 699 (1971).Google Scholar