Lattice Boltzmann Modeling of Subcontinuum Energy Transport in Crystalline and Amorphous Microelectronic Devices

Numerical simulations of time-dependent energy transport in semiconductor thin films are performed using the lattice Boltzmann method applied to phonon transport. The discrete lattice Boltzmann method is derived from the continuous Boltzmann transport equation assuming first gray dispersion and then nonlinear, frequency-dependent phonon dispersion for acoustic and optical phonons. Results indicate that a transition from diffusive to ballistic energy transport is found as the characteristic length of the system becomes comparable to the phonon mean free path. The methodology is used in representative microelectronics applications covering both crystalline and amorphous materials including silicon thin films and nanoporous silica dielectrics. Size-dependent thermal conductivity values are also computed based on steady-state temperature distributions obtained from the numerical models. For each case, reducing feature size into the subcontinuum regime decreases the thermal conductivity when compared to bulk values. Overall, simulations that consider phonon dispersion yield results more consistent with experimental correlations.

[1]  Cristina H. Amon,et al.  Boltzmann transport equation-based thermal modeling approaches for hotspots in microelectronics , 2006 .

[2]  Cristina H. Amon,et al.  Comparison of Different Phonon Transport Models for Predicting Heat Conduction in Silicon-on-Insulator Transistors , 2005 .

[3]  Cristina H. Amon,et al.  Submicron heat transport model in silicon accounting for phonon dispersion and polarization , 2004 .

[4]  R. Escobar,et al.  Lattice-Boltzmann modeling of sub-continuum energy transport in Silicon-on-Insulator microelectronics including phonon dispersion effects , 2004, The Ninth Intersociety Conference on Thermal and Thermomechanical Phenomena In Electronic Systems (IEEE Cat. No.04CH37543).

[5]  Jeng-Rong Ho,et al.  Lattice Boltzmann study on size effect with geometrical bending on phonon heat conduction in a nanoduct , 2004 .

[6]  A. Majumdar,et al.  Nanoscale thermal transport , 2003, Journal of Applied Physics.

[7]  Cristina H. Amon,et al.  Simulation of Unsteady Small Heat Source Effects in Sub-Micron Heat Conduction , 2001 .

[8]  M. Kaviany,et al.  Effects of phonon pore scattering and pore randomness on effective conductivity of porous silicon , 2000 .

[9]  Kenneth E. Goodson,et al.  Sub-Continuum Simulations of Heat Conduction in Silicon-on-Insulator Transistors , 1999, Heat Transfer: Volume 3.

[10]  A. Hunt,et al.  Theoretical modeling of carbon content to minimize heat transfer in silica aerogel , 1995 .

[11]  Bo Han,et al.  Anharmonic thermal resistivity of dielectric crystals at low temperatures. , 1993, Physical review. B, Condensed matter.

[12]  Arun Majumdar,et al.  Transient ballistic and diffusive phonon heat transport in thin films , 1993 .

[13]  A. Majumdar Microscale Heat Conduction in Dielectric Thin Films , 1993 .

[14]  C. Rüssel,et al.  Oxinitride glasses in the system MgAlSiON, prepared with the aid of an electrochemically derived polymeric precursor☆ , 1992 .

[15]  X. Lu,et al.  Optimization of monolithic silica aerogel insulants , 1992 .

[16]  Kenneth E. Goodson,et al.  Heat Transfer Regimes in Microstructures , 1992 .

[17]  Pohl,et al.  Thermal conductivity of amorphous solids above the plateau. , 1987, Physical review. B, Condensed matter.

[18]  P. Liley,et al.  Thermal Conductivity of the Elements , 1972 .

[19]  Cristina H. Amon,et al.  Multi-length and time scale thermal transport using the lattice Boltzmann method with application to electronics cooling , 2006 .

[20]  C. Amon,et al.  Thermal Transport Network Model for High-Porosity Materials: Application to Nanoporous Aerogels , 2005 .

[21]  A. McGaughey,et al.  Integration of Molecular Dynamics Simulations and Boltzmann Transport Equation in Phonon Thermal Conductivity Analysis , 2003 .

[22]  S. R. Mathur,et al.  Ballistic-Diffusive Approximation for Phonon Transport Accounting for Polarization and Dispersion , 2003 .

[23]  R. Escobar,et al.  Sub-Continuum Heat Conduction in Electronics Using the Lattice Boltzmann Method , 2003 .

[24]  J. Boon The Lattice Boltzmann Equation for Fluid Dynamics and Beyond , 2003 .

[25]  C. Amon,et al.  Design of a Low-Cost Infrared Sensor Array Through Thermal System Modeling , 2003 .

[26]  R. Escobar,et al.  Time-Dependent Simulations of Sub-Continuum Heat Generation Effects in Electronic Devices Using the Lattice Boltzmann Method , 2003 .

[27]  C. Amon,et al.  Effect of Sub-Continuum Energy Transport on Effective Thermal Conductivity in Nanoporous Silica (Aerogel) , 2003 .

[28]  Timothy S. Fisher,et al.  Application of the Lattice-Boltzmann Method to Sub-Continuum Heat Conduction , 2002 .

[29]  J. Fricke,et al.  Thermal properties of silica aerogels between 1.4 and 330 K , 1992 .

[30]  Robert O. Pohl,et al.  Lattice Vibrations and Heat Transport in Crystals and Glasses , 1988 .

[31]  J. Fricke,et al.  Aerogels — a Fascinating Class of High-Performance Porous Solids , 1986 .

[32]  J. Fricke,et al.  Infrared radiative heat transfer in highly transparent silica aerogel , 1986 .

[33]  S. Kistler The Calculation of the Surface Area of Microporous Solids from Measurements of Heat Conductivity. , 1942 .