Effect of 2D MXene-to-nanoparticle ratio on the electronic structure of Ti3C2 MXene-CsPbBr3 nanocomposites
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Updated: Feb 13, 2026

Fabrication of Ti3C2 MXene Microelectrode Arrays for In Vivo Neural Recording
Published on: February 12, 2020
1Department of Physics, Midnapore College (Autonomous), Raja Bazar Main Rd, 721101 Midnapore, W.B., India. abhijit.bera@midnaporecollege.ac.in.
Abstract:
MXene-CsPbBr3 nanocomposites have garnered significant interest for next-generation optoelectronics, combining tunable quantum effects with exceptional charge transport characteristics. Realizing optimal functionality, however, necessitates precise control over the 2D MXene-to-nanoparticle ratio. Herein, we systematically elucidate how this ratio governs the electronic structure and charge dynamics in Ti3C2 MXene-CsPbBr3 nanocomposites using scanning tunnelling spectroscopy (STS), electrostatic force microscopy (EFM), and Kelvin probe force microscopy (KPFM). STS reveals distinct density of states for isolated CsPbBr3 nanoparticles chemically bonded to MXene compared to aggregated counterparts. Schottky junctions at well-defined interfaces promote charge separation, whereas nanoparticle aggregation induces defect-mediated states, narrowing the CsPbBr3 bandgap and opening a gap in Ti3C2. Correlated EFM-KPFM analyses further demonstrate that isolated nanoparticles yield uniform electrostatics and homogeneous surface potentials, while aggregates generate localized fields and patchy work-function distributions. These results demonstrate that nanoscale electrostatics and interfacial coupling critically dictate carrier dynamics, enabling the rational design of tunable optoelectronic device architectures.
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