An open-cage bis[60]fulleroid as electron transport material for tin halide perovskite solar cells
Chemical Communications Royal Society of Chemistry (RSC) (2024)
Abstract:
Halide homogenization for low energy loss in 2-eV-bandgap perovskites and increased efficiency in all-perovskite triple-junction solar cells
Nature Energy Springer Nature 9:1 (2023) 70-80
Abstract:
Monolithic all-perovskite triple-junction solar cells have the potential to deliver power conversion efficiencies beyond those of state-of-art double-junction tandems and well beyond the detailed-balance limit for single junctions. Today, however, their performance is limited by large deficits in open-circuit voltage and unfulfilled potential in both short-circuit current density and fill factor in the wide-bandgap perovskite sub cell. Here we find that halide heterogeneity—present even immediately following materials synthesis—plays a key role in interfacial non-radiative recombination and collection efficiency losses under prolonged illumination for Br-rich perovskites. We find that a diammonium halide salt, propane-1,3-diammonium iodide, introduced during film fabrication, improves halide homogenization in Br-rich perovskites, leading to enhanced operating stability and a record open-circuit voltage of 1.44 V in an inverted (p–i–n) device; ~86% of the detailed-balance limit for a bandgap of 1.97 eV. The efficient wide-bandgap sub cell enables the fabrication of monolithic all-perovskite triple-junction solar cells with an open-circuit voltage of 3.33 V and a champion PCE of 25.1% (23.87% certified quasi-steady-state efficiency).Stabilizing non-IPR C2(13333)-C74 cage with Lu2C2/Lu2O: the importance of encaged non-metallic elements
Chemical Communications Royal Society of Chemistry (RSC) (2023)
Abstract:
Quantum-Chemical Modeling of Two Er3N@C80 Isomers
ECS Journal of Solid State Science and Technology IOP Publishing 12:9 (2023) 091004-091004
Abstract:
Computations of the molecular parameters and relative populations are reported for the two isomers of Er 3 N@C 80 experimentally known, i.e. produced by encapsulation into the isolated-pentagon-rule (IPR) C 80 cages with I h and D 5 h symmetries. The calculations are mostly based on the density-functional theory (DFT) treatments with the B3LYP functional. However, the inter-isomeric energetics is further refined with the B2PLYP method which places the D 5 h endohedral higher in the potential energy by 18.8 kcal/mol. The isomeric populations are evaluated using the Gibbs energy in a broad temperature interval. The computations performed with the floating-encapsulate-model (FEM) treatment agree with the observation that Er 3 N@ I h (7)-C 80 represents the major isomer. The calculations also suggest some similarity between Er 3 N@C 80 and Lu 3 N@C 80 so that Er 3 N@C 80 could possibly also produce a useful nanowire, like recently found with Lu 3 N@C 80 and its interesting electrical-conductivity and switching behavior.Crystallographic Characterization of Lu2O@Cs(6)‐C82 and Er2O@Cs(6)‐C82: The Role of Metal Species on Cluster Configuration†
Chinese Journal of Chemistry Wiley 41:16 (2023) 1915-1920