Tunable Chemochromism and Elastic Properties in Intercalated MoO<sub>3</sub>: Au-, Cr-, Fe-, Ge-, Mn-, and Ni-MoO<sub>3</sub>.

Reed, Bryan W; Chen, Ethan; Koski, Kristie J · ACS Nano · 2024

basic_science · Level V

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Abstract

Chemical tunability of the elastic constants of α-MoO<sub>3</sub>, a two-dimensional layered oxide, is demonstrated with mutability on the order of tens of GPa, simply by choice of a metal intercalant including Au, Cr, Fe, Ge, Mn, and Ni. Using Brillouin laser light scattering from confined acoustic phonons in nanometer-thick materials, the in-plane angular dispersion of the quantized acoustic phonon branches of 2D layered, intercalated MoO<sub>3</sub> is measured and used to determine the bulk modulus (<i>K</i>), Young's moduli (<i>E</i><sub>11</sub>, <i>E</i><sub>22</sub>, and <i>E</i><sub>33</sub>), each of the nine independent elastic tensor elements (<i>c</i><sub><i>ij</i></sub>), and the thickness. Intercalation of metals generally reduces the anisotropy in MoO<sub>3</sub> except in Ge-MoO<sub>3</sub>, for which the in-plane longitudinal elastic anisotropy is unaffected. Chemochromism from transparent white (MoO<sub>3</sub> and Fe-MoO<sub>3</sub>) to near black (Ni-MoO<sub>3</sub>) to brilliant dark blue (Ge-MoO<sub>3</sub>) is demonstrated and is associated with a reduction in electronic band gap with intercalation and an increase in absorption >600 nm for some intercalants (Cr-, Ge-, and Mn-MoO<sub>3</sub>).