Article ID Journal Published Year Pages File Type
1490055 Materials Research Bulletin 2012 9 Pages PDF
Abstract

A detailed calculation of lattice thermal conductivity of freestanding Wurtzite GaN nanowires with diameter ranging from 97 to 160 nm in the temperature range 2–300 K, was performed using a modified Callaway model. Both longitudinal and transverse modes are taken into account explicitly in the model. A method is used to calculate the Debye and phonon group velocities for different nanowire diameters from their related melting points. Effect of Gruneisen parameter, surface roughness, and dislocations as structure dependent parameters are successfully used to correlate the calculated values of lattice thermal conductivity to that of the experimentally measured curves. It was observed that Gruneisen parameter will decrease with decreasing nanowire diameters. Scattering of phonons is assumed to be by nanowire boundaries, imperfections, dislocations, electrons, and other phonons via both normal and Umklapp processes. Phonon confinement and size effects as well as the role of dislocation in limiting thermal conductivity are investigated. At high temperatures and for dislocation densities greater than 1014 m−2 the lattice thermal conductivity would be limited by dislocation density, but for dislocation densities less than 1014 m−2, lattice thermal conductivity would be independent of that.

Graphical abstractTemperature dependence of calculated lattice thermal conductivity of Wurtzite GaN nanowires.Figure optionsDownload full-size imageDownload as PowerPoint slideHighlights► A modified Callaway model is used to calculate lattice thermal conductivity of Wurtzite GaN nanowires. ► A direct method is used to calculate phonon group velocity for these nanowires. ► 3-Gruneisen parameter, surface roughness, and dislocations are successfully investigated. ► Dislocation densities are decreases with the decrease of wires diameter.

Related Topics
Physical Sciences and Engineering Materials Science Ceramics and Composites
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