{ "id": "1603.05286", "version": "v1", "published": "2016-03-16T21:30:12.000Z", "updated": "2016-03-16T21:30:12.000Z", "title": "Thermal Conductivity of Suspended Graphene with Defects", "authors": [ "Hoda Malekpour", "Pankaj Ramnani", "Srilok Srinivasan", "Ganesh Balasubramanian", "Denis L. Nika", "Ashok Mulchandani", "Roger Lake", "Alexander A. Balandin" ], "comment": "23 pages, 6 figures", "categories": [ "cond-mat.mes-hall", "cond-mat.mtrl-sci" ], "abstract": "We investigate the thermal conductivity of suspended graphene as a function of the density of defects, ND, introduced in a controllable way. Graphene layers are synthesized using chemical vapor deposition, transferred onto a transmission electron microscopy grid, and suspended over ~7.5-micrometer size square holes. Defects are induced by irradiation of graphene with the low-energy electron beam (20 keV) and quantified by the Raman D-to-G peak intensity ratio. As the defect density changes from 2.0x10^10 cm-2 to 1.8x10^11 cm-2 the thermal conductivity decreases from ~(1.8+/-0.2)x10^3 W/mK to ~(4.0+/-0.2)x10^2 W/mK near room temperature. At higher defect densities, the thermal conductivity reveals an intriguing saturation behavior at a relatively high value of ~400 W/mK. The thermal conductivity dependence on defect density is analyzed using the Boltzmann transport equation and molecular dynamics simulations. The results are important for understanding phonon - point defect scattering in two-dimensional systems and for practical applications of graphene in thermal management.", "revisions": [ { "version": "v1", "updated": "2016-03-16T21:30:12.000Z" } ], "analyses": { "keywords": [ "suspended graphene", "raman d-to-g peak intensity ratio", "transmission electron microscopy grid", "higher defect densities", "thermal conductivity decreases" ], "note": { "typesetting": "TeX", "pages": 23, "language": "en", "license": "arXiv", "status": "editable" } } }