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10. Appendix

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Chapter 6 705<br />

Strain-induced birefringence and intrinsic birefringence of cubic<br />

semiconductors<br />

Equation (6.158) describes the effect of an electric field on the dielectric function.<br />

A similar tensor equation can be used to describe the effect of a tensorial<br />

strain. Whereas a cubic crystal is usually assumed to be optically isotropic, a<br />

finite wavevector q breaks this isotropy (p. 246 and Refs. [6.7, 8]). This effect<br />

has recently received attention as determining the resolution of lenses used<br />

for uv lithography. In the past few years ab initio calculations of strain induced<br />

and q induced birefringence have been performed:<br />

G. Bester, X. Wu, D. Vanderbilt and A. Zunger: Importance of Second order<br />

Piezoelectric Effects in Zinc-Blende Semiconductors. Phys. Rev. Lett. 96,<br />

187602–187605 (2006)<br />

J. H. Burnett, Z. H Levine and E. L. Shirley: Photoelastic and Elastic Properties<br />

of the Fluorite Structure Materials, LiF and Si. Phys. Rev. B68,<br />

155120/1–12 (2003); erratum: Phys. Rev. B70, 239904 (2004).<br />

J. H. Burnett, Z. H. Levine and E. L. Shirley: Intrinsic Birefringence in calcium<br />

fluoride and barium fluoride. Phys. Rev. B64, 241102/1–4 (2001).<br />

Optical Response of Semiconductor Surfaces<br />

During the past decade many studies have concentrated on the optical response<br />

of surfaces. This is due to advances in ab initio computational techniques<br />

as well as development of highly sensitive experimental methods based<br />

on ellipsometry and reflectometry. The results have proven to be useful for<br />

the in situ characterization of epitaxial layers during growth.<br />

The calculations are often performed on fictitious samples obtained by repetition<br />

of thin layers so as to generate in the computer a three-dimensional<br />

crystal. Many experiments are of the reflectance difference variety, which take<br />

advantage of the fact that even on cubic crystals some surfaces (e.g. (110)) are<br />

anisotropic. Recent theoretical and experimental references are as follows:<br />

O. Pulci, O. Onida, R. del Sole and L. Reining: Ab Initio Calculation of Selfenergy<br />

Effects on Optical Properties of GaAs(110). Phys. Rev. Lett. 81,<br />

5374–5377 (1998).<br />

P. Chiaradia, and R. del Sole: Difference-Reflectance Spectroscopy and<br />

Reflectance-Anisotropy Spectroscopy on Semiconductor Surfaces. Surface<br />

Review and Letters 6, 517–528 (1999).<br />

W. G. Schmidt, F. Bechstedt, and J. Bernholc: Understanding Reflectance<br />

Anisotropy: Surface-State Signatures and Bulk Related Features. J. Vac. Sci.<br />

Technol. B18, 2215–2223 (2000).<br />

W. G. Schmidt, N. Esser, A. M. Frisch, P. Vogl, J. Bernholc, F. Bechstedt, M.<br />

Zorn, Th. Hannappel, S. Visbeck, F. Willig, and W. Richter: Understanding<br />

Reflectance Anisotropy: Surface-State Signatures and Bulk-Related Features<br />

in the Optical Spectrum of InP(001)(2×4). Phys. Rev. B61, R16335–8 (2000).

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