2020
DOI: 10.1016/j.actamat.2020.02.040
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Anisotropic thermal conductivity tensor of β-Y2Si2O7 for orientational control of heat flow on micrometer scales

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Cited by 14 publications
(6 citation statements)
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“…The estimated steady-state temperature increase is ∼2 K. The fwhm spatial resolution of this technique is ≈2.2 μm (Figure S5). This technique has been used previously to measure spatially inhomogeneous thermal conductivity in polycrystalline diamond, lithium-intercalated MoS 2 , and other materials. ,,, …”
Section: Methodsmentioning
confidence: 99%
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“…The estimated steady-state temperature increase is ∼2 K. The fwhm spatial resolution of this technique is ≈2.2 μm (Figure S5). This technique has been used previously to measure spatially inhomogeneous thermal conductivity in polycrystalline diamond, lithium-intercalated MoS 2 , and other materials. ,,, …”
Section: Methodsmentioning
confidence: 99%
“…This technique has been used previously to measure spatially inhomogeneous thermal conductivity in polycrystalline diamond, 19 lithium-intercalated MoS 2 , 2 and other materials. 14,29,41,42 Molecular Dynamics Simulations. Interatomic interactions are modeled with empirical potentials tested to reproduce the vibrational properties of graphite, MoS 2 , and aluminum.…”
Section: Methodsmentioning
confidence: 99%
“…At the nanoscale, heat flow must navigate length scales intrinsic to material heterogeneities. This process contributes to the macroscopic thermal properties of a material but is typically aggregated into bulk parameters that can obfuscate microscopic origins. It is well-known that, in the cases of electronic and mass transport, heterogeneity has impacts beyond a simple reduction in diffusivity, leading to fundamentally different transport regimes such as subdiffusive behavior. Subdiffusion refers to a mean-squared expansion of an initially localized heat distribution evolving as t α , where α < 1, , such that the effective thermal conductivity falls off as a power law with the length scale traversed, tending to zero in the infinite limit .…”
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confidence: 99%
“…The challenge of measuring nanoscale heat transport in heterogeneous media is that it requires a direct indicator of heat flow on the length and time scales of the encounters with nanoscale defects. , Typically, thermal conductivity is measured on length scales orders of magnitude greater than the size of individual defects, yielding an average quantity. Ultrafast optical pump–probe measurements of thin films do not typically image heat spreading, and length-dependent steady-state thermal resistance measurements lack dynamical information and require constraining sample geometries and mechanical properties .…”
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confidence: 99%
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