In the past decade, fabrication of lead halide perovskites solar cells1,2,3,4,5,6 has effectively highlighted the excellent properties of this semiconductor material, including long carrier diffusion lengths7,8,9,10, compositional tunability4,5,11 and low-cost synthesis12. In particular, the unique nature of defect tolerance13,14 makes lead halide perovskites fundamentally different from other semiconductors and thus highly promising for next-generation optoelectronic applications.
In addition to solar cells, lead halide perovskites have been shown to make excellent optoelectronic devices such as light-emitting diodes6,15,16,17,18,19,20,21,22, lasers23,24,25, and photodetectors26,27,28. Especially, when prepared in the form of colloidal nanocrystals18,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43, lead halide perovskites may exhibit strong quantum- and dielectric-confinement, large exciton binding energy44,45, and bright luminescence17,19 along with facile solution processability. Various reported geometries including quantum dots29,30,31,32, nanorods33,34 and nanoplatelets18,35,36,37,38,39,40,41,43 further demonstrate the shape tunability of lead halide perovskite nanocrystals.
Among those nanocrystals, colloidal two-dimensional (2D) lead halide perovskites, or “perovskite nanoplatelets”, are especially promising for light-emitting applications due to strong confinement of charge carriers, large exciton binding energy reaching up to hundreds of meV44, and spectrally narrow emission from thickness-pure ensembles of nanoplatelets39. Additionally, anisotropic emission reported for 2D perovskite nanocrystals46 and other 2D semiconductors47,48 highlights the potential of maximizing outcoupling efficiency from perovskite nanoplatelet-based light-emitting devices.
Here, we demonstrate a protocol for the simple, universal, room-temperature synthesis of colloidal lead halide perovskite nanoplatelets via a ligand-assisted reprecipitation technique36,38,49. Perovskite nanoplatelets incorporating iodide and/or bromide halide anions, methylammonium or formamidinium organic cations, and variable organic surface ligands are demonstrated. Procedures for controlling the absorption and emission energy and the thickness purity of the colloidal dispersion are discussed.