from Part III - Dynamical Properties
Published online by Cambridge University Press: aN Invalid Date NaN
We analyse the energy derivatives in terms of atomic displacements. We derive the interatomic force constants tensor, and from there we obtain the dynamical matrix. We introduce the phonons as quanta of atomic motion in crystals. They are obtained by diagonalization of the dynamical matrix. To comprehensively grasp phonons, we employ the quasiharmonic approximation, limiting energy development to second-order terms. Phonons are defined by their wavevectors and frequencies, governing their orientation and energy, respectively. Unlike particles, they are quasi-particles and follow Bose–Einstein statistics as bosons.
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