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. 2023 Sep 21;3(6):475–481. doi: 10.1021/acsnanoscienceau.3c00027

Figure 3.

Figure 3

(Top) Raman of Bi2Se3, Si2Te3, MoO3 nanoribbons, MoO3 ribbons, GeS, and (bottom) change in wavenumber shift from the unintercalated material. No new Raman peaks are observed. The Raman modes stiffen or soften with intercalation following similar investigations.7