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Ph.D. thesis (pdf) - dirac

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Chapter 8<br />

Boson Peak<br />

The low energy vibrations in crystalline solids are often quite well accounted for<br />

by the Debye model. In the Debye model the modes are assumed to be plane<br />

waves and the number of possible modes are counted in the Q-space. This leads<br />

to a density of vibrational states which is proportional to the square of the mode<br />

frequency g D (ω) ∝ ω 2 . It is this dependence of the vibrational density of states<br />

which leads to the well known T 3 dependence of the heat capacity in solids at low<br />

temperatures. The Debye model is described in textbooks on solid states physics<br />

and thermodynamics e.g. [Kittel, 1996; Bairlein, 1999].<br />

Disordered solids, on the other hand, have an excess in the vibrational density of<br />

states as compared to the ω 2 Debye behavior followed by crystals in the corresponding<br />

frequency range (approx 2 meV - 10 meV depending on system). The excess<br />

gives rise to a peak in the reduced density of vibrational states g(ω)/ω 2 (rDOS) and<br />

the peak is seen directly in incoherent inelastic neutron spectra, which essentially<br />

probes g(ω)/ω 2 as well as in Raman scattering spectra. The excess also gives rise<br />

to a peak in the reduced low temperature heat capacity c P (T)/T 3 .<br />

The boson peak has been studied intensively experimentally as well as theoretically<br />

over the last decade, but its origin is still controversial. The proposed explanations<br />

for the boson peak fall in three categories. (i) Localized (harmonic) modes in soft<br />

potentials (SPM), the concept of soft localized soft modes being expressed differently<br />

in different models [Gurevich et al., 2003, 2005; Klinger, 1999, 2001]. (ii) Quasilocalized<br />

sound like modes in structural regions of the nanometer size in the glass<br />

[Duval et al., 1990; Schroeder et al., 2004; Quitmann and Soltwisch, 1998], and (iii)<br />

Fluctuating elastic constants (FEC) giving rise to a peak in g(ω)/ω 2 [Maurer and<br />

Schirmacher, 2004]. The total density of vibrational states is in the two first cases<br />

described by Debye modes plus extra modes, which are ascribed to the disorder.<br />

141

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