2022
DOI: 10.1021/acs.nanolett.2c01819
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Atomic-Void van der Waals Channel Waveguides

Abstract: Layered van der Waals materials allow creating unique atomic-void channels with subnanometer dimensions. Coupling light into these channels may further advance sensing, quantum information, and single molecule chemistries. Here, we examine theoretically limits of light guiding in atomic-void channels and show that van der Waals materials exhibiting strong resonances, excitonic and polaritonic, are ideally suited for deeply subwavelength light guiding. We predict that excitonic transition metal dichalcogenides … Show more

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Cited by 11 publications
(10 citation statements)
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“…[22] However, they still have strong exciton resonances at K or K' valleys, [27] which results in high dielectric constants near the exciton energies. [28] Therefore, numerous types of passive photonic components have been proposed and investigated both theoretically [29,30] and experimentally. Experimentally demonstrated components include photonic crystals, [31][32][33][34] Mie resonators, [35][36][37][38] metalenses, [39] and whispering gallery cavities.…”
Section: Introductionmentioning
confidence: 99%
“…[22] However, they still have strong exciton resonances at K or K' valleys, [27] which results in high dielectric constants near the exciton energies. [28] Therefore, numerous types of passive photonic components have been proposed and investigated both theoretically [29,30] and experimentally. Experimentally demonstrated components include photonic crystals, [31][32][33][34] Mie resonators, [35][36][37][38] metalenses, [39] and whispering gallery cavities.…”
Section: Introductionmentioning
confidence: 99%
“…[ 5,11–13 ] At even lower energies (longer wavelengths) where the refractive index remains large but the material's absorption coefficient quickly vanishes, these materials can be exploited for lossless waveguiding and light confinement. [ 12–19 ] Furthermore, all TMDs are naturally anisotropic due to their vdW nature, endowing them with an inherent optical uniaxial permittivity with εxx=εyyεzz$\varepsilon _{xx}=\varepsilon _{yy}\ne \varepsilon _{zz}$. [ 8,13,14,17,20 ] In certain materials (e.g., in ReS 2 ) a distortion of the planar hexagonal lattice leads to biaxial anisotropy with different values of the in‐plane permittivity tensor elements, that is, εxxεyy$\varepsilon _{xx}\ne \varepsilon _{yy}$ and both being different from the out‐of‐plane εzz$\varepsilon _{zz}$.…”
Section: Introductionmentioning
confidence: 99%
“…In this regard, careful testing and optimization of the fabrication procedures, applicable not only for semiconducting but also for metallic TMDs, and tested on various challenging to work with substrates, are of particular interest. This fabrication‐oriented progress, together with theoretical efforts [ 16,18,19 ] and knowledge of basic optical constants, [ 13 ] is essential for the development of all‐TMD nanophotonics.…”
Section: Introductionmentioning
confidence: 99%
“…However, further miniaturization of photonic devices meets fundamental limitations imposed by the wave nature of light . Plasmonics was previously considered a very promising approach to overcoming these limitations, yet absorption losses become increasingly severe in highly confined plasmonic modes and resonances. With the moderate progress in overcoming the losses using excitonic materials, the attention has been shifted to new photonic materials and all-dielectric platforms …”
mentioning
confidence: 99%