Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
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 />
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