Abstract
Compared to other extrinsic phonon scattering mechanisms such as surface and interior defects, phonon scattering and lattice thermal resistance due to structural rippling in few-layer two-dimensional (2D) materials are under-examined. Here, the temperature-dependent basal-plane thermal conductivities (κ) of one rippled and four flat molybdenum disulfide (MoS2) samples are measured using a four-probe thermal transport measurement method. A flat 18 nm thick sample and a rippled 20 nm thick sample show similar peak κ values of 122 ± 17 and 129 ± 19 W m-1 K-1, respectively. In comparison, a 32 nm thick flat sample has a peak κ value of only 58 ± 11 W m-1 K-1 despite having an increased thickness. The peak thermal conductivities of the five samples decrease with increasing integrated Raman intensity caused by defects in the frequency range of the phonon bandgap in MoS2. In conjunction with the experimental findings, theoretical calculations of the temperature-, thickness-, strain-, and defect-dependent κ of thin MoS2 layers reveal the importance of interior defect scattering over scattering from compression-induced ripples and surface defects in these samples. The results further clarify the conditions where ripples are important in determining the basal plane thermal resistance in layered systems.
Original language | English |
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Article number | 221902 |
Journal | Applied Physics Letters |
Volume | 114 |
Issue number | 22 |
DOIs | |
State | Published - Jun 3 2019 |
Funding
We thank David Choi, Sean Sullivan, and Evan Fleming for assistance in AFM, Raman spectroscopy, and fast Fourier transform data analysis, respectively. The thermal transport measurements of four samples were completed with support from U.S. Office of Naval Research Award No. N00014-16-1-2798. Thermal transport measurements of the fifth sample, all Raman measurements, and the manuscript preparation were completed with support from U.S. Department of Energy, Office of Science, Basic Energy Sciences Award No. DE-FG02-07ER46377. The first principles calculations conducted by L.L. were supported by the U. S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. We acknowledge use of Texas Nanofabrication Facilities supported by the NSF NNCI Award No. 1542159.
Funders | Funder number |
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U. S. Department of Energy | |
U.S. Office of Naval Research | |
National Science Foundation | 1542159 |
U.S. Department of Energy | |
Office of Science | |
Basic Energy Sciences | |
Division of Materials Sciences and Engineering |