Tailoring Phonon-Driven Responses in α-MoO<sub>3</sub> through Isotopic Enrichment.
basic_science · Level V
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- Record sourced from PubMed, PMID 42273746.
- Also identified by DOI 10.1002/adma.73629.
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Abstract
The implementation of polaritonic materials into nanoscale devices requires selective tuning of parameters to realize desired spectral or thermal responses. One robust material, α-MoO<sub>3</sub>, an orthorhombic crystal boasting three distinct phonon dispersions, provides three polaritonic dispersions of hyperbolic phonon polaritons (HPhPs) across the mid-infrared (MIR). Here, the tunability of both optical and thermal responses in isotopically enriched α-MoO<sub>3</sub> (<sup>98</sup>MoO<sub>3,</sub> Mo<sup>18</sup>O<sub>3</sub>, and <sup>98</sup>Mo<sup>18</sup>O<sub>3</sub>) is explored. A uniform ∼5% spectral redshift from <sup>18</sup>O enrichment is observed in both Raman- and IR-active TO phonons. Both the in- and out-of-plane thermal conductivities for the isotopic variations are reported. Ab initio calculations both replicate experimental findings and analyze the select-mode three-phonon scattering contributions. The HPhPs from each isotopic variation are probed with s-SNOM, and we report an HPhP Q-factor maxima increase in <sup>98</sup>Mo<sup>18</sup>O<sub>3</sub> of ∼50% along the [100] in the RB<sub>2</sub> and ∼100% along the [001] in the RB<sub>3</sub> with respect to <sup>98</sup>MoO<sub>3</sub>. Observations in both real and Fourier space of higher-order HPhP modes propagating in slabs of isotopically enriched α-MoO<sub>3</sub> without the use of a subdiffractional surface scatterer are presented here. This work establishes the dual-element isotope enrichment of α-MoO<sub>3</sub> as an intrinsic strategy to design optical, thermal, and polaritonic properties.