A simple efficient method of nanofilm-on-bulk-substrate thermal conductivity measurement using Raman thermometry

•First Raman thermometric measurement of thermal conductivity of films on bulk substrate.•A simple efficient method: a dozen of films on quartz can be examined in one hour.•The method works for any film with thickness h > Λ (phonon-mean-free path).•For h < Λ, this method works when the in-plan...

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Published in:International journal of heat and mass transfer Vol. 123; pp. 137 - 142
Main Authors: Poborchii, Vladimir, Uchida, Noriyuki, Miyazaki, Yoshinobu, Tada, Tetsuya, Geshev, Pavel I., Utegulov, Zhandos N., Volkov, Alexey
Format: Journal Article
Language:English
Published: Oxford Elsevier Ltd 01.08.2018
Elsevier BV
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ISSN:0017-9310, 1879-2189
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Summary:•First Raman thermometric measurement of thermal conductivity of films on bulk substrate.•A simple efficient method: a dozen of films on quartz can be examined in one hour.•The method works for any film with thickness h > Λ (phonon-mean-free path).•For h < Λ, this method works when the in-plane diffusive phonon transport dominates. In contrast to known Raman-thermometric measurements of thermal conductivity (k) of suspended Si nano-membranes, here we apply Raman thermometry for k measurement of mono- and nano-crystalline Si films on quartz, which is important for applications in thermoelectricity and nanoelectronics. Experimentally, we measure linear dependence of the laser-induced Raman band downshift, which is proportional to the moderate heating ΔT, on the laser power P. Then we convert the downshift to ΔT and determine the ratio ΔT/P. The actual power absorbed by the film is calculated theoretically and controlled experimentally by the reflection/transmission measurement. Then we calculate ΔTcalc/P for arbitrary film k assuming diffusive phonon transport (DPT). Film k is determined from the condition ΔT/P = ΔTcalc/P. We show that this method works well for films with thickness h > Λ, where Λ is phonon-mean-free path, even for low-k films like nano-crystalline Si and SiGe. For h < Λ, despite ballistic phonon transport contribution, this approach works when the in-plane DPT dominates, e.g. in Si films on quartz with h ≥ 60 nm. We also show that the influence of thermal boundary resistance on the determined k is negligible at this condition. The proposed method is simple and time efficient, as dozen of films can be examined in one hour.
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ISSN:0017-9310
1879-2189
DOI:10.1016/j.ijheatmasstransfer.2018.02.074