2017
DOI: 10.1002/crat.201700114
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Inorganic Crystals with Glass‐Like and Ultralow Thermal Conductivities†

Abstract: The ability to control the transport of thermal energy is critical in a wide variety of technologies. At the same time, understanding the underlying microscopic mechanisms of thermal transport in solids continues to be a central goal of condensed matter and materials physics, with many persistent challenges and unanswered questions. One of the remarkable findings has been the observation that some crystalline materials have very low, glass-like thermal conductivities despite long-range order in the arrangement… Show more

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Cited by 75 publications
(56 citation statements)
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“…The contribution of C V to thermal conductivity was limited, as C V of each atom approached 3k B at temperature beyond Debye temperature . Therefore, Λ could be obtained based on Equation and:…”
Section: Methodsmentioning
confidence: 99%
“…The contribution of C V to thermal conductivity was limited, as C V of each atom approached 3k B at temperature beyond Debye temperature . Therefore, Λ could be obtained based on Equation and:…”
Section: Methodsmentioning
confidence: 99%
“…For macroscale applications in which films inevitably become large enough that grains of varying orientations form, thermal conductivity reduction in one crystallographic direction does not have significant benefit. Thus, for isotropic crystals, such reduction is typically achieved via increasing compositional disorder, which can lead to mass mismatch, atomic radii mismatch, and local atomic strain that results in additional phonon scattering. For example, mixed crystals with controlled disorder were shown to have thermal conductivities that approach their minimum limit .…”
Section: Thermal and Physical Properties Of Esos At Room Temperaturementioning
confidence: 99%
“…Dense materials have shown the lowest κ in the range of 1 to 2 W m −1 K −1 at high temperature, as represented by the amorphous limit discussed in Section 2. Κ lower than the amorphous limit, commonly referred to as "ultralow" κ, [106] has also been observed in a few classes of fully dense materials, for instance, in multilayer with nanoscale interfaces or nanolaminates, disordered layered crystals of WSe 2 , [107] and thin films of MoSe 2 , [108] and layered heterostructures. [109] For these materials, κ is still higher than that of air (e.g., 0.026 W m −1 K −1 at 25 °C and 1 atm).…”
Section: High-temperature Thermal Transport In Porous Materialsmentioning
confidence: 99%