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Quantum Confined High-Entropy Lanthanide Oxysulfide Colloidal Nanocrystals

[Image: see text] We have synthesized the first reported example of quantum confined high-entropy (HE) nanoparticles, using the lanthanide oxysulfide, Ln(2)SO(2), system as the host phase for an equimolar mixture of Pr, Nd, Gd, Dy, and Er. A uniform HE phase was achieved via the simultaneous thermol...

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Detalles Bibliográficos
Autores principales: Ward-O’Brien, Brendan, McNaughter, Paul D., Cai, Rongsheng, Chattopadhyay, Amrita, Flitcroft, Joseph M., Smith, Charles T., Binks, David J., Skelton, Jonathan M., Haigh, Sarah J., Lewis, David J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9614967/
https://www.ncbi.nlm.nih.gov/pubmed/36194549
http://dx.doi.org/10.1021/acs.nanolett.2c01596
Descripción
Sumario:[Image: see text] We have synthesized the first reported example of quantum confined high-entropy (HE) nanoparticles, using the lanthanide oxysulfide, Ln(2)SO(2), system as the host phase for an equimolar mixture of Pr, Nd, Gd, Dy, and Er. A uniform HE phase was achieved via the simultaneous thermolysis of a mixture of lanthanide dithiocarbamate precursors in solution. This was confirmed by powder X-ray diffraction and high-resolution scanning transmission electron microscopy, with energy dispersive X-ray spectroscopic mapping confirming the uniform distribution of the lanthanides throughout the particles. The nanoparticle dispersion displayed a significant blue shift in the absorption and photoluminescence spectra relative to our previously reported bulk sample with the same composition, with an absorption edge at 330 nm and a λ(max) at 410 nm compared to the absorption edge at 500 nm and a λ(max) at 450 nm in the bulk, which is indicative of quantum confinement. We support this postulate with experimental and theoretical analysis of the bandgap energy as a function of strain and surface effects (ligand binding) as well as calculation of the exciton Bohr radiii of the end member compounds.