10. Appendix
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Chapter 8 711<br />
Strain Shift Coefficients in Si1xGex Alloys. J. Appl. Phys. 103, 093521/1–4<br />
(2008).<br />
General Reading<br />
M. Cardona and G. Güntherodt (Eds.), Light Scattering in Solids VII: Crystal<br />
Field and Magnetic Excitations, (Springer, Heidelberg, 2000).<br />
M. Cardona and G. Güntherodt (Eds.), Light Scattering in Solids VIII:<br />
Fullerenes, Semiconductor Surfaces, Coherent Phonons, (Springer, Heidelberg,<br />
2000).<br />
M. Cardona and R. Merlin (Eds.), Light Scattering in Solids IX: Novel Materials<br />
and Techniques, (Springer, Heidelberg, 2007).<br />
V.G. Plekhanov, Applications of the Isotopic Effect in Solids (Springer, Heidelberg,<br />
2004).<br />
Chapter 8<br />
Photoelectron spectroscopy<br />
During the past two decades the number of electron synchrotrons and storage<br />
rings dedicated exclusively to applications of synchrotron radiation has<br />
proliferated. Most of these applications involve condensed matter physics, especially<br />
semiconductors. Most developed and a few developing countries (e.g.<br />
Brazil) have either domestic synchrotrons or easy access to one in a neighboring<br />
country. Their light and x-rays emission, once monochromatized, is particularly<br />
suitable for photoelectron spectroscopy. Although Chapter 8 discusses<br />
mostly bulk photoemission spectroscopy, a few pages are already devoted to<br />
surface effects. During the past decade emphasis has shifted from bulk to surface<br />
phenomena, a field in which ab initio electronic and vibronic calculations<br />
have been very helpful. The availability of synchrotrons has also made possible<br />
the development of a bulk-type spectroscopy in which electrons are resonantly<br />
excited from a core level to a conduction band. X-rays of a lower<br />
energy are then emitted through recombination of valence electrons with the<br />
hole left behind in the core. The efficiency of this Raman-like spectroscopy<br />
(called resonant x-ray emission spectroscopy) is rather limited and so is the<br />
corresponding resolution. Nevertheless, it allows one to map out the full band<br />
structures and even obtain information about their atomic and orbital compositions.<br />
As already mention in the past editions of this book, scanning tunneling<br />
microscopies and spectroscopies are useful techniques to elucidate surface<br />
properties. Some recent references are listed below.<br />
A. M. Frisch, W. G. Schmidt, J. Bernholc, M. Privstovsek, N. Esser, W. Richter:<br />
(2×4) GaP(001) Surfaces: Atomic Structure and Optical Anisotropy. Phys.<br />
Rev. B60, 2488–2494 (1999).