International Workshop on Energy Conversion and Information Processing Devices, Nice, France Monte Carlo phonon transport at nanoscales Karl Joulain, Damian Terris, Denis Lemonnier Laboratoire d’études thermiques, ENSMA, Futuroscope France David Lacroix LEMTA, Univ Henri Poincaré, Nancy, France 1/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Random walk and diffusion equation QuickTime™ et un décompresseur TIFF (non compressé) sont requis pour visionner cette image. 2/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France RW and diffusion equation Einstein 1905 Density of particle at x and t. Probability to travel on a distance between x and x+dx during t 3/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France RW and diffusion equation Density at time t+t Density expansion 4/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France RW and diffusion equation Diffusion equation 100000 particles at the origin at t=0. After 40 jumps: 5/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Nanoscale conductive heat transfer Distribution function Boltzmann Equation Relaxation time approximation 6/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Boltzmann equation resolution methods • Kinetic theory • Radiative transfer equation methods – P1 – Discrete ordinate • Monte Carlo methods Advantages – Geometry – Separation of relaxation times 7/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Monte Carlo simulation Earlier work : Peterson (1994), Mazumder and Majumdar (2001) System divided in cells Phonon energy and number in cells 8/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Initialization Weight Too many phonons Spectral discretization Nb spectral bins Distribution function Phonons drawn in cell until Polarization Direction Two numbers drawn to choose de phonon direction 9/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Drift and scattering Drift Phonon scattering Relaxation time t due to anharmonic processes and impurities Modified distribution function 10/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Boundary conditions Temperature imposed at both end of the system Extrem cells are phonon blackbodies Boundary scattering Diffuse or specular reflexion at boundaries Crystal dispersion 11/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Transient results in bulk Bulk simulation : specular reflection at boundaries Diffusion regime Phys. Rev. B, 72, 064305 (2005) 12/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Results in bulk Ballistic regime Diffusion balistic regime transtion Phys. Rev. B, 72, 064305 (2005) 13/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Nanowires Boundary collisions : purely diffuse Appl. Phys. Lett, 89, 103104 (2006) 14/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Perspectives Mode resolution for nanowires Relaxation times •No collision at lateral boundaries t 1 2 •Impurities • Anharmonic interactions => new estimation of t 15/16 International Workshop on Energy Conversion and Information Processing Devices, Nice, France Perspectives • 1D kinetic theory. • 1D direct integration of Boltzmann equation. • 1D Monte Carlo simulations. • 3D integration of Boltzmann equation by discrete ordinate method. 16/16
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