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10. Appendix

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706 <strong>Appendix</strong> D<br />

J. Pollmann, P. Kruger, A. Mazur, and M. Rohlfing: Electron, Phonon and Excitons<br />

at Semiconductor Surfaces in Advances in Solid State Physics, Volume<br />

42 (Springer, Berlin, Heidelbery, 2002) 189–206.<br />

W. G. Schmidt, K. Seino, P. H. Hahn, F. Bechstedt, W. Lu, S. Wang, and J.<br />

Bernholc: Calculation of Surface Optical Properties: from Qualitative Understanding<br />

to Quantitative Predictions. Thin Solid Films, 455–456, 764–771<br />

(2004).<br />

P. Weightman, D. S. Martin, R. J. Cole, and T. Farrell: Reflection Anisotropy<br />

Spectroscopy. Rep. Prog. Phys. 68, 1251–1341 (2005).<br />

L. F. Lastras-Martínez, J. M. Flores-Camacho, A. Lastras-Martínez, R. E.<br />

Balderas-Navarro and M.Cardona: Measurement of the Surface Strain Induced<br />

by Reconstructed Surfaces of GaAs(001) using Photoreflectance and<br />

Reflectance-Difference Spectroscopies. Phys. Rev. Letters 96, 047402–047405<br />

(2006).<br />

M. Marsili, O. Pulci, F. Fuchs, F. Bechstedt, and R. del Sole: Many Body Effects<br />

in the Electronic and Optical Properties of the (111) Surface of Diamond.<br />

Surface Science 601, 4097–4101 (2007).<br />

K. F. Mak, M. Y. Sfeir, Y. Wu, C. H. Lui, J. A. Misewich, and T. F. Heinz: Measurement<br />

of the Optical Conductivity of Graphene. Phys. Rev. Lett. 101,<br />

196405–196408 (2008).<br />

Dielectric Response due to Vibrational Excitations:<br />

Born Effective Charges<br />

The first order infrared absorption related to the excitation of phonons in polar<br />

materials is discussed in Sect. 6.4. Its strength is related to the Born effective<br />

charge e ∗ shown in Eq. (6.119). This effective charge has been calculated<br />

for many semiconductors during the past 15 years using ab initio techniques.<br />

e ∗ and other polarization related properties have been described by several<br />

authors using the so-called Berry’s phase. Ab initio methods also allow the<br />

calculation of the dependence of e ∗ on strain. Although a non-zero e ∗ is characteristic<br />

of polar crystals and thus vanishes for crystalline Si, in amorphous<br />

Si deviations from the regular lattice positions induce dynamic charges and,<br />

consequently, ir absorption. Several references are listed as follows.<br />

R. Resta: Macroscopic Polarization in Crystalline Dielectrics: the Geometric<br />

Phase Approach. Rev. Mod. Physics 66, 899–915 (1994).<br />

A. Debernardi, M. Bernasconi, M. Cardona, and M. Parrinello: Infrared Absorption<br />

in Amorphous Silicon from ab initio Molecular Dynamics. Appl.<br />

Phys. Lett. 71, 2692–2694 (1997).<br />

X. Gonze and C. Y. Lee: Dynamical Matrices, Born Effective Charges, Dielectric<br />

Permittivity Tensors, and Interatomic Force Constants from Density<br />

Functional Theory. Phys. Rev. B55, 10355–10368 (1997).<br />

F. Bernardini, V. Fiorentini, and D. Vanderbilt: Accurate Calculation of Polarization<br />

Related Quantities in Semiconductors. Phys. Rev. B63, 193201/1–4<br />

(2001).

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