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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)

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