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GaAs Heteroepitaxy on Fluoride by Electron Beam Induced Surface Modification

Published online by Cambridge University Press:  17 March 2011

Tobias Fritz
Affiliation:
Swiss Federal Institute of Technology (ETH) Physics Department / Institute of Quantum Electronics ETH Zurich Hoenggerberg – HPT, CH-8093 Zurich, Switzerland
Markus Haiml
Affiliation:
Swiss Federal Institute of Technology (ETH) Physics Department / Institute of Quantum Electronics ETH Zurich Hoenggerberg – HPT, CH-8093 Zurich, Switzerland
Silke Schön
Affiliation:
Swiss Federal Institute of Technology (ETH) Physics Department / Institute of Quantum Electronics ETH Zurich Hoenggerberg – HPT, CH-8093 Zurich, Switzerland
Ursula Keller
Affiliation:
Swiss Federal Institute of Technology (ETH) Physics Department / Institute of Quantum Electronics ETH Zurich Hoenggerberg – HPT, CH-8093 Zurich, Switzerland
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Abstract

GaAs saturable absorber materials are used in ultrafast nonlinear optics to obtain all-optical switching in optoelectronic devices. They are introduced to semiconductor saturable absorber mirrors (SESAMs) for the generation of ultrashort laser pulses. GaAs is grown on CaF2 by molecular beam epitaxy to fabricate devices, which provide a large high reflection bandwidth. The CaF2 surface was exposed to high- and low-energy electron irradiation before and during growth to increase the surface free energy for the subsequent GaAs overgrowth. A three-layer GaAs/ fluoride device was designed and fabricated to study the impact of the electron exposure on the growth mode and the surface roughness. The surface morphology of an optoelectronic device can cause nonsaturable losses, which degrade the device performance. Therefore, the effect of the electron exposure of the CaF2 layer on the surface roughness of the device was studied by atomic force microscopy. Measurements of the scattered light from the device surface allowed for a quantitative analysis of the nonsaturable losses attributed to the surface morphology of the device.

Type
Research Article
Copyright
Copyright © Materials Research Society 2002

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References

1. Keller, U., Miller, D.A.B., Boyd, G.D., Chiu, T.H., Ferguson, J.F., and Asom, M.T., Opt. Lett. 17, 505 (1992).Google Scholar
2. Schön, S., Haiml, M., and Keller, U., Appl. Phys. Lett. 77, 782 (2000).Google Scholar
3. Schön, S., Zogg, H., and Keller, U., J. Cryst. Growth 201–202, 1020 (1999).Google Scholar
4. Schön, S., Haiml, M., Gallmann, L., and Keller, U., J. Cryst. Growth 227–228, 172 (2001).Google Scholar
5. Schön, S., Gallmann, L., Haiml, M., and Keller, U., in OSA Trends in Optics and Photonics (TOPS) 56, (Optical Society of America, Washington DC, USA, 2001), pp. 314.Google Scholar
6. Schön, S., Haiml, M., Achermann, M., and Keller, U., J. Vac. Sci. Technol. B18, 1701 (2000).Google Scholar
7. Hwang, S. M., Miyasato, K., Kawasaki, K., and Tsutsui, K., Jpn. J. Appl. Phys. 35, 1701 (1996).Google Scholar
8. Paulus, M., and Martin, O.J.F., J. Opt. Soc. Am. A18, 854 (2001).Google Scholar
9. Paulus, M., private communications.Google Scholar
10. Bennewitz, R., Smith, D., and Reichling, M., Phys. Rev. B59, 8237 (1999).Google Scholar
11. Reichling, M., Nucl. Instr. Meth. Phys. Res. B101, 108 (1995).Google Scholar
12. Reichling, M., Wilson, R.M., Bennewitz, R., Williams, R.T., Gogoll, S., Stenzel, E., and Matthias, E. Surf. Sci. 366, 531 (1996).Google Scholar