Transition metal dichalcogenides have emerged as promising materials for nano-photonic resonators due to their large refractive index, low absorption within the visible spectrum and compatibility with a wide variety of substrates. Here we use these properties to fabricate WS$_2$ monomer and dimer nano-antennas in a variety of geometries enabled by the anisotropy in the crystal structure. Using dark field spectroscopy, we reveal multiple Mie resonances, including anapole modes, for which we show polarization-sensitive second harmonic generation in the dimer nano-antennas. We introduce post-fabrication atomic force microscopy repositioning and rotation of dimer nano-antennas, achieving gaps as small as 10$pm$5 nm and opening a host of potential applications. We further studied these structures with numerical simulations yielding electric field intensity enhancements of >10$^3$ corresponding to Purcell factors as high as 157 for emitters positioned within the nano-antenna hotspots. Optical trapping simulations of small dimer gaps yield attractive forces of >350 fN for colloidal quantum dots and > 70 fN for protein-like, polystyrene beads. Our findings highlight the advantages of using transition metal dichalcogenides for nano-photonics by exploring new applications enabled by their unique properties.
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