2020
DOI: 10.1103/physrevb.102.205405
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Heat current anticorrelation effects leading to thermal conductivity reduction in nanoporous Si

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Cited by 13 publications
(19 citation statements)
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References 46 publications
(67 reference statements)
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“…Accordingly, the running thermal conductivity κ (τ ) first increases with increasing τ , then develops a maximum value at τ max , and eventually decays to zero from the positive side, with fluctuations in the long-time limit due to increasing noise-to-signal ratio. Such 035417-3 peaks in the running thermal conductivity have been observed in other contexts, such as thermal transport in nanoporous silicon [33] and nonlocal thermal transport within the linearresponse formalism [34].…”
Section: Resultssupporting
confidence: 55%
“…Accordingly, the running thermal conductivity κ (τ ) first increases with increasing τ , then develops a maximum value at τ max , and eventually decays to zero from the positive side, with fluctuations in the long-time limit due to increasing noise-to-signal ratio. Such 035417-3 peaks in the running thermal conductivity have been observed in other contexts, such as thermal transport in nanoporous silicon [33] and nonlocal thermal transport within the linearresponse formalism [34].…”
Section: Resultssupporting
confidence: 55%
“…Accordingly, the running thermal conductivity κ(τ ) first increases with increasing τ , then develops a maximum value at τ max , and eventually decays to zero from the positive side, with fluctuations in the long-time limit due to increasing noise-to-signal ratio. Such peaks in the running thermal conductivity have been observed in other contexts, such as thermal transport in nanoporous silicon [32] and nonlocal thermal transport within the linear-response formalism [33].…”
Section: Models and Methodssupporting
confidence: 53%
“…Nanoengineered membranes including thin films, 2,3 nanowires, 4 nanomeshes, 5,6 nanocomposites, 7,8 and nanoporous structures [9][10][11][12] feature extremely low thermal conductivity, sometimes beyond the amorphous limit. 13 This is largely due to the scattering of phonons with large MFPs (generally with small frequencies), i.e., those that are comparable with the characteristic length of the material.…”
Section: Introductionmentioning
confidence: 99%
“…13 This is largely due to the scattering of phonons with large MFPs (generally with small frequencies), i.e., those that are comparable with the characteristic length of the material. Low-thermal conductivity can also be obtained with point defects 14,15 , such as those induced by alloying, 13,16 and vacancies 12 . Point-defect scattering strongly suppresses medium-to high-frequency phonons, mostly with shorter MFPs while leaving low-frequency phonons (generally with longer MFPs) unimpeded.…”
Section: Introductionmentioning
confidence: 99%