研究目的
To understand the formation of Eu3+ in nanocrystals of CsPbX3 (X = Cl, Br) and the occurrence of f-f transitions in Eu3+ doped nanocrystals for light emitting diodes.
研究成果
The presence of surface oxygen is the most likely reason for the observation of Eu3+ in nanolayers of CsPbBr3, making f-f transitions possible. A similar behavior has been obtained in Eu doped nanolayers of CsPbCl3. The doping of Eu in nanolayers of CsPbBr3 leads to almost no change in the atomic structure and the cost of doping Eu atom in the orthorhombic layer is very small (~ 0.175 eV). Therefore, doping of Eu and similarly other rare earths is very interesting for achieving bright luminescence from this new family of semiconductors.
研究不足
The study is limited to theoretical calculations and does not include experimental validation. The size of nanocrystals in experimental studies is rather large (~7 nm), which is difficult to study theoretically, hence a slab of CsPbBr3 (~1.8 nm thick) was considered which also has strong surface effects similar to NCs.
The study involves ab initio calculations on nanolayers of CsPbBr3 doped with Eu to explore the possibility of the existence of Eu in 3+ state. Various possibilities were considered including the presence of a Cs vacancy near Eu, presence of interstitial H or OH around Eu, substituting O in place of surface Br attached with Eu, and attaching extra halogen with Eu. The calculations were performed using plane wave projector augmented wave (PAW) pseudopotential method as implemented in Vienna Ab initio Simulation Package (VASP). The exchange-correlation functional was treated within generalized gradient approximation (GGA) of Perdew, Burke, and Ernzerhof (PBE). Structural optimization and total energy calculations of the doped and undoped nanolayers were performed using 2x2x1 k-points mesh for cubic and orthorhombic phases. On-site Coulomb interactions were included for Eu doped systems using GGA+U method and by taking U= 6 eV for the f electrons. Spin-orbit interactions were included for the heavy elements Pb and Eu along with spin-polarised effects.
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