3D Anisotropic Thermal Conductivity of Exfoliated Rhenium Disulfide

ReS₂ represents a different class of 2D materials, which is characterized by low symmetry having 1D metallic chains within the planes and extremely weak interlayer bonding. Here, the thermal conductivity of single-crystalline ReS₂ in a distorted 1T phase is determined at room temperature for the in-plane directions parallel and perpendicular to the Re-chains, and the through-plane direction using time-domain thermoreflectance. ReS₂ is prepared in the form of flakes having thicknesses of 60–450 nm by micromechanical exfoliation, and their crystalline orientations are identified by polarized Raman spectroscopy. The in-plane thermal conductivity is higher along the Re-chains, (70 ± 18) W m⁻¹ K⁻¹, as compared to transverse to the chains, (50 ± 13) W m⁻¹ K⁻¹. As expected from the weak interlayer bonding, the through-plane thermal conductivity is the lowest observed to date for 2D materials, (0.55 ± 0.07) W m⁻¹ K⁻¹, resulting in a remarkably high anisotropy of (130 ± 40) and (90 ± 30) for the two in-plane directions. The thermal conductivity and interface thermal conductance of ReS₂ are discussed relative to the other 2D materials.

The 3D thermal-conductivity tensor of ReS₂, a transition-metal dichalcogenide with Re-chains on the plane, is determined using time-domain thermoreflectance. The thermal conductivity is higher along the Re-chains, 70 W m⁻¹ K⁻¹, compared to transverse to the chains, 50 W m⁻¹ K⁻¹. The through-plane thermal conductivity is the lowest observed for 2D materials, 0.55 W m⁻¹ K⁻¹.

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