(1963). D.T. Morelli, G.A. Slack, in: S.L. Shindé, J.S. Goela (Eds.), High Therm. Conduct. Mater., Springer, New York, 2006, pp. 37–68. Fig. from X. Qian, J. Zhou, G. Chen, Nat. Mater. (2021) G.A. Slack, J. Phys. Chem. Solids 34 (1973) 321–335. Лекция «Введение в физику полупроводников» / 9 августа 2022 г. 9 Lattice thermal conductivity Based on Leibfried and Schlömann model (lately corrected by Slack), the lattice thermal conductivity at high temperature 𝑇 > 𝜃𝐷 : 𝜅𝑙𝑎𝑡 = 𝐴 𝑘𝐵 𝜃𝐷 ℏ 3 ഥ 𝑀𝛿 𝛾2𝑁𝐴𝑣 𝑛 Τ 5 3𝑇 where 𝑁𝐴𝑣 is the Avogadro constant, 𝑛 is the number of atoms in the unit cell (molecule), 𝛿3 = 𝑉𝑎𝑡, 𝑉𝑎𝑡 is the average volume per atom, 𝐴 = 𝑓 𝛾 . Thus, several rules for low thermal conductivity can be formulated: (1) high mass of constituent atoms ( ഥ 𝑀𝛿𝜃𝐷 3 is maximized for light mass); (2) weak interatomic bonding; (3) complex crystal structure; (4) high anharmonicity. Conditions (1) and (2) means a low 𝜃𝐷, condition (3) means high 𝑛, and condition (4) means high 𝛾.