“…In crystalline structures, Umklapp scattering dominates the phonon transport at the temperature range of interest, which shortens the phonon mean free path and leads to a reduction in the thermal conductivity with the temperature. The thermal conductivity of crystalline samples κ C is computed using the Callaway model 44 , which is expressed aswhere the average phonon relaxation time τ is computed combining phonon-grain boundary , film boundaries , phonon-impurity , Umklapp , phonon-carrier , and, in the case of Ag 3.9 Sb 33.6 Te 62.5 films, nanoprecipitate scattering mechanisms as 45–47 , where D is the average grain size , P is the phonon transmission across the grain boundary, t is the thickness of the film, n NP is the nanoprecipitate number density, and Θ is the average nanoprecipitate scattering cross-section, which is estimated using the average nanoinclusion size, and the mass and tensor strength difference with the matrix 17,48 . As detailed at the beginning of this section, the thickness of the film is measured using cross-sectional SEM imaging and the grain size is derived from the XRD spectra.…”