Publication date: 15th December 2025
Copper sulfide (CuS) semiconductor nanoparticles exhibit localized surface plasmon resonances in the near-infrared (NIR) range via vacancy-induced charge carriers [1], enabling plasmon-assisted enhancement of photoluminescence of quantum dots (QDs) [2]. Periodic plasmonic structures can simultaneously raise excitation fields [3], increase radiative decay rates (via Purcell effect) [4], and decouple emission into well-defined angles via hybrid plasmonic modes. Periodic metal plasmonic nanostructures [4-6] as well as lithography-processed Si-based metasurfaces [7] are reported to enhance and direct the spontaneous emission of NIR QDs. An alternative approach for metasurfaces preparation is laser interference lithography [8], which allows scalable and reproducible grating fabrication for controllable directional light extraction from nanoparticle arrays.
In this work, we designed a mask‑compatible CuS semiconductor stripe grating that can enhance and redirect NIR (800–1300 nm) QD emission. CuS hexagonal nanoplatelets were densely packed into stripes with a period of 600−900 nm, thickness of 40 nm, and width of 90 nm on a glass substrate. The particles were first drop-cast from their concentrated colloidal solution and then were shaped into regular stripes on top of a 10 nm thick CuS nanoparticle layer with the use of a soft polydimethylsiloxane mask. The grating morphology was investigated with atomic force microscopy. For simulations we used Ansys Lumerical FDTD software with periodic Bloch boundary conditions for in‑plane symmetry and perfectly matched layers above and below the structure. Plane‑wave excitation was used with polarization oriented across the stripes and monitors were placed before and after the structure to collect its reflection and transmission power, respectively. Field maps around stripes demonstrate the enhancement of electromagnetic field distribution around the structure. Simulations predict lattice–assisted plasmon resonance hybridization with 2–5-fold radiative‑rate enhancement and more than 3-fold local field enhancement due to efficient coupling.
