Organic Semiconductors with Halogenated Quinoid Terminals for Sensitive Short‐Wave Infrared Detection and Imaging

T Tengfei Li (Yusuf Hamied Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom) Y Youyi Qu (State Key Laboratory of Silicon and Advanced Semiconductor Materials School of Materials Science and Engineering Zhejiang University Hangzhou China) Y Yingchen Peng (State Key Laboratory of Physical Chemistry of Solid Surfaces, College of Chemistry and Chemical Engineering) H Heng Liu Y Yujie Yang (Key Laboratory of Colloid and Interface Chemistry of the Ministry of Education, School of Chemistry and Chemical Engineering, Shandong University) J Jianqi Zhang (Key Laboratory of Nanosystem and Hierarchical Fabrication) H Huiqing Hou (Beijing National Laboratory for Molecular Sciences, CAS Key Laboratory of Organic Solids, Institute of Chemistry) L Lei Li Q Qianqian Lin X Xinhui Lu (Department of Physics) Y Ye Yang Y Yanjun Fang Y Yuze Lin (Beijing National Laboratory for Molecular Sciences, CAS Key Laboratory of Organic Solids, Institute of Chemistry)

Abstract

ABSTRACT Short‐wave infrared (SWIR) detection and imaging is vital for optoelectronics, and solution‐processed organic semiconductors pave the way for developing large‐area, cost‐effective SWIR sensor arrays compatible with readout integrated circuits through facile pattern‐free processing. However, limited by the energy gap law, molecular skeleton vibrations, especially high‐frequency stretching modes like C─H bonds, induce accelerated non‐radiative decay in SWIR molecules, making the performance of SWIR organic photodetectors (OPDs), particularly in the long‐wavelength region, still lag behind that of commercial inorganic counterparts. Here we develop an efficient molecular engineering strategy to construct vibration‐suppressed SWIR molecules by employing halogenated quinoid terminals. Relative to their analogs with H atoms, halogenated semiconductors show attenuated exciton‐vibration coupling, decreased conformation and energy disorder, as well as enhanced intramolecular charge transfer, resulting in nearly doubled exciton lifetimes and reduced energy disorder from 103 to 66–83 meV, accompanied by 0.1–0.15 eV optical bandgap narrowing. The optimized SWIR OPDs achieve broadband photoresponse (0.3–1.6 µm) and high specific detectivities up to 2.11 × 10 11 Jones at 1.03 µm, overwhelming all reported OPDs with >1.4 µm response and comparable to Ge photodetectors in 0.9–1.4 µm range. Furthermore, we demonstrate an advanced active‐matrix OPD‐based SWIR imaging system prototype, showcasing applicability in diverse SWIR scenarios.

Article Details

Volume / Issue Vol. 1, Issue 1
Published January 24, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (13)

T

Tengfei Li

Yusuf Hamied Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom

Y

Youyi Qu

State Key Laboratory of Silicon and Advanced Semiconductor Materials School of Materials Science and Engineering Zhejiang University Hangzhou China

Y

Yingchen Peng

State Key Laboratory of Physical Chemistry of Solid Surfaces, College of Chemistry and Chemical Engineering

H

Heng Liu

Y

Yujie Yang

Key Laboratory of Colloid and Interface Chemistry of the Ministry of Education, School of Chemistry and Chemical Engineering, Shandong University

J

Jianqi Zhang

Key Laboratory of Nanosystem and Hierarchical Fabrication

H

Huiqing Hou

Beijing National Laboratory for Molecular Sciences, CAS Key Laboratory of Organic Solids, Institute of Chemistry

L

Lei Li

Q

Qianqian Lin

X

Xinhui Lu

Department of Physics

Y

Ye Yang

Y

Yanjun Fang

Y

Yuze Lin

Beijing National Laboratory for Molecular Sciences, CAS Key Laboratory of Organic Solids, Institute of Chemistry