10. Appendix
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Chapter 3 695<br />
Inelastic x-ray Scattering (IXS)<br />
As discussed in Chap. 7, laser Raman scattering yields very precise information<br />
about the frequencies and line widths of phonons at or near the center of<br />
the Brillouin zone. However, it cannot access phonons throughout the whole<br />
Brillouin zone because the laser wavelength is much larger than the typical lattice<br />
constants. The measured dispersion relations shown in this chapter were<br />
obtained by inelastic neutron scattering (INS), taking advantage of the fact<br />
that the wavelength of thermal neutrons is close to the lattice constants. This<br />
technique, however, is slow, cumbersome, requires large samples and has poor<br />
energy resolution. Within the past decade, these problems have been circumvented<br />
(except for the poor resolution) by using IXS, with monochromatized<br />
x-rays from a synchrotron radiation source. An example of these measurements<br />
is given in Fig. 3.3. IXS allows the use of small samples ( 1mmin<br />
size) and is thus suitable for measurements under pressure in diamond anvil<br />
cells (DAC). A discussion can be found in the following articles:<br />
M. Krisch: Status of Phonon Studies at High Pressure by inelastic X-ray scattering.<br />
J. Raman Spectr. 34, 628–632 (2003).<br />
M. Krisch and F. Sette: Inelastic X-ray Scattering from Phonons, in Light Scattering<br />
in Solids IX, edited by M.Cardona and R. Merlin (Springer, Heidelberg,<br />
2007) p. 317–369.<br />
Effects of Hydrostatic Pressure on Phonons<br />
The large samples required by INS limits the highest hydrostatic pressure that<br />
can be reached to about 1 GPa. With IXS much smaller samples can be used<br />
and, with the help of DACs pressures as high as a few hundred GPa can be<br />
reached at the expense of the resolution. The pressure effects of main interest<br />
are the shift in phonon frequencies (related to the mode Grüneisen parameters<br />
discussed in Problem 3.17) and changes in phonon line widths. These “anharmonic”<br />
effects are amenable to ab initio calculations. The phase transitions<br />
which take place at high pressures are also evinced in the phonon spectra.<br />
Recent advances in the field can be found in the following publications:<br />
A. Debernardi: Anharmonic Èffects in the Phonons of III-V Semiconductors:<br />
First Principles Calculations. Solid State Commun. 113, 1–10 (1999).<br />
J. Camacho, K. Parlinski, A. Cantarero, and K. Syassen: Vibrational Properties<br />
of the high pressure Cmcm phase of ZnTe. Phys. Rev. B70, 033205–033208<br />
(2004).<br />
J. Kulda, A. Debernardi, M. Cardona, F. de Geuser, and E. E. Haller: Self-<br />
Energy of Zone- Boundary Phonons in Germanium: Ab initio Calculations<br />
versus Neutron Spin-Echo Measurements. Phy. Rev. B69, 045209–045213<br />
(2004).<br />
J. Serrano, A. H. Romero, F. J. Manjon, R. Lauck, M. Cardona and A. Rubio:<br />
Pressure Dependence of the Lattice Dynamics of ZnO, an ab initio approach.<br />
Phys. Rev. B69, 094306–094319 (2004). (ABINIT)