Local Atomic Off‐Centering Mediated Efficient Self‐Trapped Excitonic Emission in Cs <sub>5</sub> Cu <sub>3</sub> Cl <sub>6</sub> I <sub>2</sub> Nanoplates

A Anustoop Das (New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India) J Jayita Pradhan (New Chemistry Unit Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR) Jakkur P.O. Bengaluru 560064 India) S Simanta Kalita (Chemistry and Physics of Materials Unit) K Kaushik Kundu (New Chemistry Unit Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR) Jakkur P.O. Bengaluru 560064 India) P Paribesh Acharyya (Department of Chemistry) S Sarit S. Agasti (New Chemistry Unit and School of Advanced Materials (SAMat), Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur, Bangalore 560064, India) K Kanishka Biswas (New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India)

Abstract

Abstract Cu(I)‐based low‐dimensional metal halides have received significant recognition attributable to their intriguing optoelectronic properties, which instigate the emergence of self‐trapped excitons (STEs) accompanied by intense broadband emissions. However, fundamental crystal structural origin of such STE is still elusive. Herein, we have synthesized Cu(I)‐based mixed halide, Cs 5 Cu 3 Cl 6 I 2 nanoplates (NPs) using room temperature ligand‐assisted reprecipitation method, which showed an intense blue emission with broad line‐width, large Stokes shift, long photoluminescence lifetime, high photoluminescence quantum yield (PLQY) of ∼75%. Temperature‐dependent PL intensity and line‐width analysis unfolded strong exciton‐phonon coupling in NP sample. Synchrotron X‐ray pair distribution function analysis determines the local Cu off‐centering, which provides the required lattice anharmonicity and softness for intense STE in Cs 5 Cu 3 Cl 6 I 2 NPs. The existence of such soft lattice structure associated with low‐energy phonons was verified by sound velocity, Raman spectroscopy and low‐temperature heat capacity measurements. The fluorescence microscopy and super‐resolution optical imaging were implemented at single‐particle level which exhibited minimal temporal PL intermittency with reasonable photostability under high‐intensity illumination. Accordingly, we hypothesize that the intense broadband emission of NPs are  accompanied by the local atomic off‐centering‐driven lattice deformation during photo‐excitation process.

Article Details

Volume / Issue Vol. 64, Issue 28
Published July 07, 2025
ISSN 1433-7851
Publisher Wiley

Journal Info

Angewandte Chemie International Edition

Wiley

ISSN: 1433-7851 Physical Sciences

Authors (7)

A

Anustoop Das

New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India

J

Jayita Pradhan

New Chemistry Unit Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR) Jakkur P.O. Bengaluru 560064 India

S

Simanta Kalita

Chemistry and Physics of Materials Unit

K

Kaushik Kundu

New Chemistry Unit Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR) Jakkur P.O. Bengaluru 560064 India

P

Paribesh Acharyya

Department of Chemistry

S

Sarit S. Agasti

New Chemistry Unit and School of Advanced Materials (SAMat), Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur, Bangalore 560064, India

K

Kanishka Biswas

New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India