Monte Carlo Study of Phonon Transport in Solid Thin Films Including Dispersion and Polarization
By S. Mazumder, Arun Majumdar. 2001
463 citations recorded by the source corpus.
Subfields: Civil and Structural Engineering, Electrical and Electronic Engineering, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/9cfbbc744bd2daa3a19fbb74f68e0cf232e74691
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In Civil and Structural Engineering
- A. McGaughey
- Eric Pop
- M. Kaviany
- Kenneth E. Goodson
- Nicolas G. Hadjiconstantinou
- Jean-Philippe M. Péraud
- Gang Chen
In Electrical and Electronic Engineering
- Eric Pop
- Sanjiv Sinha
- Kenneth E. Goodson
- A. McGaughey
- Nicolas G. Hadjiconstantinou
- M. Kaviany
- Jean-Philippe M. Péraud
In Materials Chemistry
- A. McGaughey
- M. Kaviany
- Kenneth E. Goodson
- Eric Pop
- Sanjiv Sinha
- Nicolas G. Hadjiconstantinou
- Jean-Philippe M. Péraud
- Baoling Huang
Citations in the corpus
- Phonon transport in molecular dynamics simulations: Formulation and thermal conductivity prediction. (2006, methodology): “The development of relaxation time models is useful for thermal conductivity calculations as used, but will also be applicable to more general BTE calculations, including numerical solutions based on the phonon equation of radiation transfer [66] and direct simulation Monte Carlo techniques [67].”
- Energy dissipation and transport in nanoscale devices (2010, background): “Such details are important because the emitted phonons have different velocities and widely varying contributions to heat transport [52-55] and device heating [56, 57].”
- Heat Generation and Transport in Nanometer-Scale Transistors (2006, background): “1590 Proceedings of the IEEE |V ol. 94, No. 8, August 2006 dynamics [17] or microscopic phonon transport simulations [ 18 ], [19], and they offer a comprehensive look at the complexity of Joule heating in silicon.”
- Efficient simulation of multidimensional phonon transport using energy-based variance-reduced Monte Carlo formulations (2011, methodology): “However, because the frequencies of the scattered phonons are drawn randomly, conservation of energy is enforced by adding or deleting particles until a target energy is approximately reached [8, 9].”