Phonon interaction with ripples and defects in thin layered molybdenum disulfide

Brandon Smith, Lucas Lindsay, Jaehyun Kim, Eric Ou, Rui Huang, Li Shi

Research output: Contribution to journalArticlepeer-review

12 Scopus citations

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 languageEnglish
Article number221902
JournalApplied Physics Letters
Volume114
Issue number22
DOIs
StatePublished - 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.

FundersFunder number
U. S. Department of Energy
U.S. Office of Naval Research
National Science Foundation1542159
U.S. Department of Energy
Office of Science
Basic Energy Sciences
Division of Materials Sciences and Engineering

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