Abstract:We present an atomic-scale theory of interface scattering of phonons in superlattices. In particular, we describe the scattering as a result of two features, mixing of atoms at interfaces and presence of dislocations at interfaces due to lattice mismatch. We apply the theory to quantitatively explain the thermal conductivity, and its variation with period and temperature, of Si/Ge superlattices.
“…7(a) are considered. Such devices, if the Si-Ge periods are repeated as in superlattices, could exhibit very low thermal conductivities 20,49 while keeping relatively good electronic properties, thus fulfilling two important criteria needed for high performance thermogenerators. Since the maximum phonon energy in Ge is smaller than in Si (37 vs. 64 meV with the harmonic parameters of Ref.…”
Section: B Homogeneous Si Nanowiresmentioning
confidence: 99%
“…Measurement techniques have evolved to the point where they can provide a deep insight into the thermal conduction of nanowires 10,11 , which is essential for both electronic and thermoelectric applications. A the same time the theoretical understanding of the thermal properties of nanowires has kept improving due to the development of always complexer and more accurate models [12][13][14][15][16][17][18][19][20][21][22][23] . In many cases, a direct comparison of experimental data and simulation results is possible.…”
Section: Introductionmentioning
confidence: 99%
“…In spite of the computational complexity, ultra-scaled nanowires with a diameter of 3 nm, different crystal orientations (<100>, <110>, and <111>), lengths (20,40, and 60 nm), temperatures (from 50 to 1000 K), and made of more than 20000 atoms can be simulated within a couple of hours. As applications, the thermal current flowing through such nanowires as well as the resulting thermal resistance and conductivity are calculated.…”
Section: Introductionmentioning
confidence: 99%
“…However, at the nanometer scale, such approaches are no more valid and must be replaced by models treating thermal transport at the phonon level. Nowadays, most theoretical investigations of nanoscale thermal transport are based either (i) on the linearized Boltzmann Transport Equation with Fermi's Golden Rule 15,16,20,21 , (phonon quantum confinement neglected) (ii) on Equilibrium Molecular Dynamics simulations 23 (computationally very intensive and statistical average over long time periods required), (iii) on first-principle (ab-initio) methods 19 (limited to very small systems), or (iv) on coherent phonon Non-equilibrium Green's Function (NEGF) approaches 12,17,22 (no dissipative interactions). The versatility and flexibility of NEGF 25,26 make it one of the most widely-spread and appreciated formalisms to solve quantum transport problems.…”
Phonon transport is simulated in ultra-scaled nanowires in the presence of anharmonic phononphonon scattering. A modified valence-force-field model containing four types of bond deformation is employed to describe the phonon bandstructure. The inclusion of five additional bond deformation potentials allows to account for anharmonic effects. Phonon-phonon interactions are introduced through inelastic scattering self-energies solved in the self-consistent Born approximation in the Nonequilibrium Green's Function formalism. After calibrating the model with experimental data, the thermal current, resistance, and conductivity of <100>-, <110>-, and <111>-oriented Si nanowires with different lengths and temperatures are investigated in the presence of anharmonic phononphonon scattering and compared to their ballistic limit. It is found that all the simulated thermal currents exhibit a peak at temperatures around 200 K if phonon scattering is turned-on while they monotonically increase when this effect is neglected. Finally, phonon transport through Si-Ge-Si nanowires is considered.
“…7(a) are considered. Such devices, if the Si-Ge periods are repeated as in superlattices, could exhibit very low thermal conductivities 20,49 while keeping relatively good electronic properties, thus fulfilling two important criteria needed for high performance thermogenerators. Since the maximum phonon energy in Ge is smaller than in Si (37 vs. 64 meV with the harmonic parameters of Ref.…”
Section: B Homogeneous Si Nanowiresmentioning
confidence: 99%
“…Measurement techniques have evolved to the point where they can provide a deep insight into the thermal conduction of nanowires 10,11 , which is essential for both electronic and thermoelectric applications. A the same time the theoretical understanding of the thermal properties of nanowires has kept improving due to the development of always complexer and more accurate models [12][13][14][15][16][17][18][19][20][21][22][23] . In many cases, a direct comparison of experimental data and simulation results is possible.…”
Section: Introductionmentioning
confidence: 99%
“…In spite of the computational complexity, ultra-scaled nanowires with a diameter of 3 nm, different crystal orientations (<100>, <110>, and <111>), lengths (20,40, and 60 nm), temperatures (from 50 to 1000 K), and made of more than 20000 atoms can be simulated within a couple of hours. As applications, the thermal current flowing through such nanowires as well as the resulting thermal resistance and conductivity are calculated.…”
Section: Introductionmentioning
confidence: 99%
“…However, at the nanometer scale, such approaches are no more valid and must be replaced by models treating thermal transport at the phonon level. Nowadays, most theoretical investigations of nanoscale thermal transport are based either (i) on the linearized Boltzmann Transport Equation with Fermi's Golden Rule 15,16,20,21 , (phonon quantum confinement neglected) (ii) on Equilibrium Molecular Dynamics simulations 23 (computationally very intensive and statistical average over long time periods required), (iii) on first-principle (ab-initio) methods 19 (limited to very small systems), or (iv) on coherent phonon Non-equilibrium Green's Function (NEGF) approaches 12,17,22 (no dissipative interactions). The versatility and flexibility of NEGF 25,26 make it one of the most widely-spread and appreciated formalisms to solve quantum transport problems.…”
Phonon transport is simulated in ultra-scaled nanowires in the presence of anharmonic phononphonon scattering. A modified valence-force-field model containing four types of bond deformation is employed to describe the phonon bandstructure. The inclusion of five additional bond deformation potentials allows to account for anharmonic effects. Phonon-phonon interactions are introduced through inelastic scattering self-energies solved in the self-consistent Born approximation in the Nonequilibrium Green's Function formalism. After calibrating the model with experimental data, the thermal current, resistance, and conductivity of <100>-, <110>-, and <111>-oriented Si nanowires with different lengths and temperatures are investigated in the presence of anharmonic phononphonon scattering and compared to their ballistic limit. It is found that all the simulated thermal currents exhibit a peak at temperatures around 200 K if phonon scattering is turned-on while they monotonically increase when this effect is neglected. Finally, phonon transport through Si-Ge-Si nanowires is considered.
“…We discuss the veracity of this assumption later. Previous works have modeled phonon transport across heterointerfaces incorporating non-idealities such as extended chemical intermixing, 21,22,24 misfit dislocations, 19,81 and microcrystalline or amorphous regions. 21,22,25,82 In all of these previous works, changes in h K were controlled by changes in the diffusive phonon scattering events around the interface caused by these non-idealities.…”
The overarching goal of this Truman LDRD project was to explore mechanisms of thermal transport at interfaces of nanomaterials, specifically linking the thermal conductivity and thermal boundary conductance to the structures and geometries of interfaces and boundaries. Deposition, fabrication, and post possessing procedures of nanocomposites and devices can give rise to interatomic mixing around interfaces of materials leading to stresses and imperfections that could affect heat transfer. An understanding of the physics of energy carrier scattering processes and their response to interfacial disorder will elucidate the potentials of applying these novel materials to next-generation high powered nanodevices and energy conversion applications. An additional goal of this project was to use the knowledge gained from linking interfacial structure to thermal transport in order to develop avenues to control, or "tune" the thermal transport in nanosystems.4
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