2015
DOI: 10.1007/s10825-015-0773-2
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Electro-thermal simulation based on coupled Boltzmann transport equations for electrons and phonons

Abstract: To study the thermal effect in nano-transistors, a simulator based on the self-consistent solution of the Boltzmann transport equations (BTEs) for both electrons and phonons has been developed. It has been used here to investigate the self-heating effect in a 20-nm long double gate MOSFET. In this model, a Monte Carlo (MC) solver for electrons has been coupled with a direct solver for the phonon transport. This method is particularly efficient to provide a deep insight on the out-of-equilibrium thermal dissipa… Show more

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Cited by 19 publications
(7 citation statements)
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“…Semi-classical Monte Carlo simulations are also starting to emerge in TE materials [241][242][243][244][245][246][247][248]. The advantage of MC is that the computational cost increases linearly with the system size and scattering events can be incorporated relatively easily.…”
Section: Simulation Essentialsmentioning
confidence: 99%
“…Semi-classical Monte Carlo simulations are also starting to emerge in TE materials [241][242][243][244][245][246][247][248]. The advantage of MC is that the computational cost increases linearly with the system size and scattering events can be incorporated relatively easily.…”
Section: Simulation Essentialsmentioning
confidence: 99%
“…In 1D systems, the BTE can be solved by a direct approach 21 , but for 3D problems, a stochastic particle Monte Carlo method 22 is much more efficient and it is able to include complex scattering terms 23 . This versatile approach can solve accurately the BTE much beyond the linear approximation, and in complex geometries.…”
Section: Introductionmentioning
confidence: 99%
“…Previous works [2,19,20] have highlighted the doping dependence of κ(T) of a material, in addition to its temperature dependence, and modeled the same through the temperature coefficients, κ a , κ b and κ c . In this work, while extracting R THm from the experimental data using the methodology detailed in [18], we also extract the parameters α and β of an alternate thermal conductivity model, κ(T) = βT −α [21]. From these alternate model parameters, we find κ a , κ b and κ c parameters by optimization.…”
Section: Model Extension For Structures With Beol and Parameter Extractionmentioning
confidence: 99%