1988
DOI: 10.1016/0378-4363(88)90285-9
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Lattice thermal conductivity of deformed crystals

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Cited by 4 publications
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“…Nevertheless, the motion of atoms in crystalline materials turns out to be most readily described not in terms of the individual atoms, but in terms of traveling waves, which are named lattice vibrations by Born [47]. In a lattice dynamics (LD) system with a harmonic approximation, the displacement of atoms can be decomposed into a linear combination of normal modes [48], permitting only a discrete set of wavevectors. The number of allowed wavevectors is equal to the number of primitive unit cells.…”
Section: The Lattice Dynamics Formulationmentioning
confidence: 99%
“…Nevertheless, the motion of atoms in crystalline materials turns out to be most readily described not in terms of the individual atoms, but in terms of traveling waves, which are named lattice vibrations by Born [47]. In a lattice dynamics (LD) system with a harmonic approximation, the displacement of atoms can be decomposed into a linear combination of normal modes [48], permitting only a discrete set of wavevectors. The number of allowed wavevectors is equal to the number of primitive unit cells.…”
Section: The Lattice Dynamics Formulationmentioning
confidence: 99%
“…For a harmonic approximation, atomic displacements can be decomposed into a linear combination of normal modes with a discrete set of wavevectors where the number of wavevectors equals the number of unit cells [37,38]. If we only consider the contributions from short-wavelength phonons with k > k C , then the displacement of the α th particle in a unit cell at undeformed position x is given as follows:…”
Section: Lattice Dynamics Methodsmentioning
confidence: 99%