Physics and Modeling of Phonon Wave Behaviors in Nanoscale Heat Conduction

doi:10.19596/j.cnki.1001-246x.9000

Abstract

Abstract:

Nanoscale heat conduction has attracted considerable attention due to the unique transport behaviors exhibited by its intrinsic heat-carrying phonons, as well as its significant potential in addressing thermal management issues in electronic devices and enhancing thermoelectric conversion efficiency. This paper reviews the research progress in nanoscale heat conduction theory and simulations over the past three decades. It particularly introduces and discusses methods based on both wave and particle perspectives, focusing on nanoscale coherent thermal conduction mechanisms. Finally, the paper analyzes the challenges facing the field of nanoscale heat conduction research and outlines potential future directions, aiming to deepen the understanding of the wave-particle duality of heat-carrying phonons and promote their application in critical areas.

Key words: nanoscale heat conduction, coherent heat conduction, phonon thermal transport, wave effects

Bin LIU, Yunfan HUANG, Moran WANG. Physics and Modeling of Phonon Wave Behaviors in Nanoscale Heat Conduction[J]. Chinese Journal of Computational Physics, 2024, 41(6): 746-771.

Figures/Tables 9

Fig.1 Information and energy transfer by phonon spectrum[128]

Fig.2 Different types of PnCs for manipulating coherent heat conduction[60-61, 65, 67, 69, 72-73, 91-92, 128, 146]

Fig.3 (a)Schematic image of a unit period in SLs and(b)phonon dispersions of Si/Ge and GaAs/AlAs SLs[95]; (c)schematic, (d)thermal conductivity and(e)phonon dispersions of periodic and aperiodic superlattice[63]

Fig.4 (a)GaAs/AlAs SLs with constant period thickness and(b)their measured thermal conductivity[48]; (c)reflection and transmission of phonon waves at the interface and in the film and(d)calculated thermal conductance of a thin film by EWM[94]; (e)phonon energy transmission spectra of GaAs/AlAs SLs and single interface[188]

Fig.5 (a)Thermal conductivity of Si/Ge SLs with smooth and rough interfaces[174]; (b)TEM micrographs of Al/Si rough interface[204]; (c)interfacial thermal conductance of Al/Si interfaces as a function of roughness[203]

Fig.6 (a)Thermal conductivity versus length of GaAs/ AlAs SLs with different ErAs interfacial coverage[60]; (b)schematic of the genetic algorithm based optimization method[207]; (c)variation of thermal conductivity with average period thickness for periodic and aperiodic SLs[207]; (d)phonon ballistic, propagating and localized mode in aperiodic SLs[65]

Fig.7 (a)Comparison of the phonon dispersion and thermal conductivity of a pillared silicon thin film with a corresponding uniform thin film[89]; (b)schematic of silicon membrane with pillar arrays[90]; (c)phonon MFP of silicon nanowires with different structures[91]; (d)thermal conductivity of silicon nanowire cross junction[92]

Fig.8 (a)Measured thermal conductivity of CaTiO3/SrTiO3 SLs[50]; (b)thermal conductivity of graphene/hBN SLs[222]; (c)phonon decay versus correlation time in Tl3VSe4[199]; (d)theoretical and measured thermal conductivities of amorphous silicon[200]; (e)schematic of the isotopic-superlattice graphene nanoribbon and(f)its thermal conductivity[118]

Fig.9 (a)Thermal conductivity and phonon MFP of periodic and aperiodic SLs[230]; (b)phonon mean free path of bulk Si at room temperature; (c)coherent/incoherent switching frequency as a function of roughness size[243]; (d)phonon characteristic lengths involved in SLs[229]; (e)accumulated thermal conductivity of silicon as a function of phonon wavelength and MFP[97]

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