Electrons and Phonons: The Theory of Transport Phenomena in Solids
By J. Ziman. 2001
2,106 citations recorded by the source corpus.
View Paper: https://www.semanticscholar.org/paper/0d242782af0568f2cb9c9c22d2f23a96f3e5326f
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Citations in the corpus
- Giant anharmonic phonon scattering in PbTe. (2011, background): “5), while conserving phonon energy and momentum [24].”
- One-dimensional quantum liquids: Beyond the Luttinger liquid paradigm (2011, background): “ight-movers) into the excitation spectrum of free bosons. These 1D bosons are nothing but quantized waves of density of a 1D Fermi gas, and their description is identical to that of acoustic phonons (Ziman, 1960). The beauty of the encoding is that it puts the free-fermion Hamiltonian and densityden”
- Nanostructuring and High Thermoelectric Efficiency in p‐Type Ag(Pb1 – ySny)mSbTe2 + m (2006, result): “Our results indicate significant changes in the lattice dynamics of the investigated system at high temperatures deviating from the Debye–Peierls theory, which predicts a scaling law jlatt ∼ 1/T.([13]) It is interesting to note that this very low jlatt value is significantly lower that those of eith”
- Wigner Formulation of Thermal Transport in Solids (2021, methodology): “Green, Peierls’ LBTE conductivity (κP), which displays the universal T−1 asymptotics (dashed line) [28, 32, 44, 100].”
- A perspective on conventional high-temperature superconductors at high pressure: Methods and materials (2019, background): “Anharmonic effects, caused by higher-order terms in the expansion of the energy surface, introduce interactions between phonons, and thus finite scattering rates and finite lifetimes [216, 217].”
- BoltzTraP2, a program for interpolating band structures and calculating semi-classical transport coefficients (2017, methodology): “ould produce a p-type material. The BTE describes the behavior of an out-of-equilibrium system in terms of a balance between scattering in and out of each possible state, with scalar scattering rates [33]. We have implemented the linearized version of the BTE under the RTA, where the transport distr”
- Stress, strain and Raman shifts (2018, background): “phonon mode m in a crystal as a result of a strain ε is determined by a second-rank symmetric tensor, the phononmode Grüneisen tensor γm [12, 15, 16]:”
- Low effective mass leading to high thermoelectric performance (2011, background): “This is because μ∝mbmc (mc, conduction mass of the carriers) [18-20] when the carriers are predominantly scattered by acoustic phonons, as has been found in most of known and good thermoelectrics.”