2013
DOI: 10.1115/1.4024909
|View full text |Cite
|
Sign up to set email alerts
|

Combined Kinetic Monte Carlo—Molecular Dynamics Approach for Modeling Phonon Transport in Quantum Dot Superlattices

Abstract: A new kinetic Monte Carlo method for modeling phonon transport in quantum dot superlattices is presented. The method uses phonon scattering phase functions and cross sections to describe collisions between phonons and quantum dots. The phase functions and cross sections are generated using molecular dynamics simulation, which is capable of including atomistic effects otherwise unavailable in Monte Carlo approaches. The method is demonstrated for a test case featuring a Si-Ge quantum dot superlattice, and the m… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2016
2016
2016
2016

Publication Types

Select...
1
1

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(1 citation statement)
references
References 77 publications
(124 reference statements)
0
1
0
Order By: Relevance
“…[15][16][17][18][19] Generally, the MC method follows a time-splitting algorithm, namely, the dynamics of a simulated particle is decoupled into advection and scattering processes, and thus the time step used is less than the relaxation time, and the grid size is less than the phonon mean-free-path. 20 Consequently, the computational costs of MC method are expensive in the acoustic thick regime, which prohibit its applications for multiscale problems with diffusive region, although it can be quite efficient for ballistic transport. It is also noted that an improved MC method has been developed recently by simulating only the deviation from equilibrium such that the variance can be efficiently reduced in simulating systems with small temperature variations.…”
Section: Introductionmentioning
confidence: 99%
“…[15][16][17][18][19] Generally, the MC method follows a time-splitting algorithm, namely, the dynamics of a simulated particle is decoupled into advection and scattering processes, and thus the time step used is less than the relaxation time, and the grid size is less than the phonon mean-free-path. 20 Consequently, the computational costs of MC method are expensive in the acoustic thick regime, which prohibit its applications for multiscale problems with diffusive region, although it can be quite efficient for ballistic transport. It is also noted that an improved MC method has been developed recently by simulating only the deviation from equilibrium such that the variance can be efficiently reduced in simulating systems with small temperature variations.…”
Section: Introductionmentioning
confidence: 99%