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. 2018 Jun 6;8:8668. doi: 10.1038/s41598-018-26751-4

Figure 2.

Figure 2

(a) Raman spectra of the E12g peak intensity variation for few monolayers thick 2H-MoTe2 flakes exposed to 100 °C in air for the shown time intervals. (b) Comparison of E12g peak intensities changes as a function of 100 °C in air holding time for uncapped MoTe2 and BN-capped MoTe2 flakes; to facilitate the comparisons and avoid errors due to absolute peak intensity changes over time, the peak intensity was normalized to the Si substrate peak (520.5 cm−1). The shown linear fitting was used to calculate E12g peak intensity decline due to oxidation processes for 2H-MoTe2 and 2H-MoTe2/a-BN.