2015
DOI: 10.1016/j.physb.2014.11.098
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A universal T2 behavior of low temperature thermal conductivity of some simple molecular polycrystals

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Cited by 4 publications
(2 citation statements)
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“…A phenomenological analysis of the thermal conductivity for the monoclinic phase κ m ( T ) can be carried out using two competing terms which account for propagation of acoustic phonons with long relaxation times τ R (ω, T ), i.e., with mean free path larger than the lattice parameters, and for short-wavelength acoustic phonons with the minimum value of τ MIN = π/ω. Both contributions give rise to the bell-like shape for κ­( T ) in a double-log scale. Such a common maximum for a dielectric crystal features the change from an increase of the density of high-energy phonons at low-temperature to a rapid increase of intensity of three-phonon scatterings by the so-called Umklapp processes which strongly limit the thermal conductivity of the crystal. , The κ ph ( T ) or Debye term is written as where x = ℏω/ k B T, Θ D is the Debye temperature, τ R ( x ) is an effective relaxation time for phonon scattering, and c s is a sound velocity averaged over longitudinal and transverse polarizations. Values of Θ D and c s are obtained from the Debye behavior of heat capacity at low temperature.…”
Section: Discussionmentioning
confidence: 99%
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“…A phenomenological analysis of the thermal conductivity for the monoclinic phase κ m ( T ) can be carried out using two competing terms which account for propagation of acoustic phonons with long relaxation times τ R (ω, T ), i.e., with mean free path larger than the lattice parameters, and for short-wavelength acoustic phonons with the minimum value of τ MIN = π/ω. Both contributions give rise to the bell-like shape for κ­( T ) in a double-log scale. Such a common maximum for a dielectric crystal features the change from an increase of the density of high-energy phonons at low-temperature to a rapid increase of intensity of three-phonon scatterings by the so-called Umklapp processes which strongly limit the thermal conductivity of the crystal. , The κ ph ( T ) or Debye term is written as where x = ℏω/ k B T, Θ D is the Debye temperature, τ R ( x ) is an effective relaxation time for phonon scattering, and c s is a sound velocity averaged over longitudinal and transverse polarizations. Values of Θ D and c s are obtained from the Debye behavior of heat capacity at low temperature.…”
Section: Discussionmentioning
confidence: 99%
“…32,33 The κ ph (T ) or Debye term is written as 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 temperature. The contributions of the dierent phonon-scattering processes are introduced into the relaxation time τ R (x) by means of the Mattiessen's rule,…”
Section: Acs Paragon Plus Environmentmentioning
confidence: 99%