Related Experiment Video
Updated: Sep 17, 2025

Facile Synthesis of Colloidal Lead Halide Perovskite Nanoplatelets via Ligand-Assisted Reprecipitation
Published on: October 1, 2019
Plexciton Dynamics in Au-Hybrid CsPbBr3 Perovskite Nanoplatelets
Eeshani Bora1, Jugal P Das2, Subarna Samanta2
1Nano Physical Spectroscopy Group, Department of Chemistry, School of Natural Sciences, Shiv Nadar Institution of Eminence, Delhi NCR, Uttar Pradesh 201314, India.
None:
Interaction of polar excitations in quantum size particles and localized surface plasmons in metallic nanoparticles results in formation of a quasi-particle called plexciton, a coupled exciton-plasmon polariton. We report observation of thickness dependent plexcitons in Au-hybrid CsPbBr3 nanoplatelets (NPls) using optical spectroscopic measurements. Our results suggest that the greater quantum and dielectric confinement leads to extremely large exciton binding energies in thin CsPbBr3 NPls, enhancing the Fröhlich interaction. In effect, exciton-phonon scattering phenomenon dominates the exciton decay dynamics in thin NPls. Surprisingly, the exciton-phonon scattering vanishes completely on Au-incorporation in thin CsPbBr3 NPls, directing the formation of strong plexcitons by coupling between the localized surface plasmons of Au and the confined excitons in thin NPls. Here the plasmon induced electric field propagates through the NPls, thus altering the dielectric field strengths responsible for such elevated exciton binding energy and introducing additional screening effects to the excitons. In turn, the exciton binding energy reduces significantly, hindering the exciton-phonon interaction. Moreover, the weakened exciton binding energy extends the exciton lifetime and increases the free carrier yield, which shows a clear thickness dependence, highlighting their promising applications in nonlinear optoelectronics.
Related Concept Videos
Valence Bond Theory
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
Hybridization of Atomic Orbitals II

