The optical and acoustic branch of the phonon dispersion relation are displayed in the following figure:
For further simplification we approximate both branches:
The phonons with a weak dependence on \(k\) are approximated by \(\omega = const.\) (Einstein model).
The phonons with a linear dependence for small \(k\) values are approximated by \(\omega = v k \) (Debye model).
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© J. Carstensen (Stat. Meth.)