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Heat dissipation in partially perforated phononic nano-membranes with periodicities below 100 nm

Authors :
Antonin M. Massoud
Valeria Lacatena
Maciej Haras
Emmanuel Dubois
Stéphane Monfray
Jean-Marie Bluet
Pierre-Olivier Chapuis
Jean-François Robillard
Centre d'Energétique et de Thermique de Lyon (CETHIL)
Université Claude Bernard Lyon 1 (UCBL)
Université de Lyon-Université de Lyon-Institut National des Sciences Appliquées de Lyon (INSA Lyon)
Université de Lyon-Institut National des Sciences Appliquées (INSA)-Institut National des Sciences Appliquées (INSA)-Centre National de la Recherche Scientifique (CNRS)
INL - Matériaux Fonctionnels et Nanostructures (INL - MFN)
Institut des Nanotechnologies de Lyon (INL)
École Centrale de Lyon (ECL)
Université de Lyon-Université de Lyon-Université Claude Bernard Lyon 1 (UCBL)
Université de Lyon-École Supérieure de Chimie Physique Électronique de Lyon (CPE)-Institut National des Sciences Appliquées de Lyon (INSA Lyon)
Université de Lyon-Institut National des Sciences Appliquées (INSA)-Institut National des Sciences Appliquées (INSA)-Centre National de la Recherche Scientifique (CNRS)-École Centrale de Lyon (ECL)
Institut d’Électronique, de Microélectronique et de Nanotechnologie - UMR 8520 (IEMN)
Centrale Lille-Université de Lille-Centre National de la Recherche Scientifique (CNRS)-Université Polytechnique Hauts-de-France (UPHF)-JUNIA (JUNIA)
Université catholique de Lille (UCL)-Université catholique de Lille (UCL)
Microélectronique Silicium - IEMN (MICROELEC SI - IEMN)
Université catholique de Lille (UCL)-Université catholique de Lille (UCL)-Centrale Lille-Université de Lille-Centre National de la Recherche Scientifique (CNRS)-Université Polytechnique Hauts-de-France (UPHF)-JUNIA (JUNIA)
STMicroelectronics [Crolles] (ST-CROLLES)
The authors acknowledge support from INSA Lyon through BQR project MaNaTherm, EU projects QuantiHeat and ERC (Grant No. UPTEG 338179), ANR project NanoHeat, and Project NANO2017. This work was partly supported by the STMicroelectronics-IEMN common laboratory and the RENATECH French network. The authors thank Dr. S. Gomes and Dr. S. Lefevre for useful discussions and R. Bon and F. Andre for the TEM images.
Renatech Network
NANO2017
Laboratoire commun STMicroelectronics-IEMN T4
ANR-11-PDOC-0024,nanoHEAT,Mécanismes des transferts de chaleur à l'échelle nanométrique et optimisation(2011)
European Project: 604668,EC:FP7:NMP,FP7-NMP-2013-LARGE-7,QUANTIHEAT(2013)
European Project: 338179,EC:FP7:ERC,ERC-2013-StG,UPTEG(2013)
Source :
APL Materials, APL Materials, 2022, 10 (5), pp.051113. ⟨10.1063/5.0091539⟩
Publication Year :
2022
Publisher :
HAL CCSD, 2022.

Abstract

International audience; Understanding how thermal-phonon paths can be shaped is key for controlling heat dissipation at the nanoscale. Thermophononic crystals are periodic porous nanostructures with thermal conductivity deviating from effective medium theory, which is possible if the characteristic sizes are of the order of phonon mean free paths and/or if phonons are forced to flow in privileged directions. We investigate suspended silicon nanomembranes with a periodic array of partially perforated holes of original paraboloid shape, with all characteristic lengths below 100 nm. Results from scanning thermal microscopy, a thermal sensing technique derived from atomic force microscopy, indicate that partial perforation of the membranes impacts heat conduction moderately, with the holey crystals showing a thermal conductivity reduction by a factor 6 in comparison to the bulk and a factor 2.5 in comparison to the non-perforated membrane. The impact of the phononic shapes is analyzed in light of a complementary Monte Carlo ray-tracing estimate of the effective phonon mean free paths that include multiple phonon reflection and highlights phonon backscattering.

Details

Language :
English
ISSN :
2166532X
Database :
OpenAIRE
Journal :
APL Materials, APL Materials, 2022, 10 (5), pp.051113. ⟨10.1063/5.0091539⟩
Accession number :
edsair.doi.dedup.....1b3f5f1d1165d501ad5797fd9ec2fa1c
Full Text :
https://doi.org/10.1063/5.0091539⟩