Non‐Contact Dipole Moment Electric Modulation Achieving High Performance Near‐Infrared Organic Photodetectors

X Xue Shi J Jia‐Wei Qiao (School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan Shandong 250100 P. R. China) J Jin‐Qun Xu (School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan Shandong 250100 P. R. China) P Peng Lu (The ZeoMat Group, Key Laboratory of Photoelectric Conversion and Utilization of Solar Energy, Qingdao New Energy Shandong Laboratory) H Hao Wang (Division of Quantitative Sciences, Department of Oncology Johns Hopkins University School of Medicine Baltimore Maryland USA) X Xin‐Xin Xia (National Engineering Research Center for Colloidal Materials, Key Laboratory of Special Functional Aggregated Materials (Shandong University), Ministry of Education, School of Chemistry & Chemical Engineering Shandong University Jinan Shandong 250100 P. R. China) M Mao‐Jie Zhang (National Engineering Research Center for Colloidal Materials, Key Laboratory of Special Functional Aggregated Materials (Shandong University), Ministry of Education, School of Chemistry & Chemical Engineering Shandong University Jinan Shandong 250100 P. R. China) K Kai‐Wen Meng (State Key Lab of Crystal Materials Shandong University Jinan 250100 P. R. China) G Gang Lian (State Key Laboratory of Crystal Materials Shandong University Jinan P.R. China) X Xiao‐Yan Du (School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan Shandong 250100 P. R. China) H Hang Yin X Xiao‐Tao Hao (School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan People's Republic of China)

Abstract

Abstract Near‐infrared (NIR) detectors, serving as critical technological nodes bridging microscopic molecular recognition and macroscopic intelligent perception, meet the demands of cutting‐edge technologies such as multispectral imaging. Organic semiconductor materials demonstrate unique advantages for NIR organic photodetectors (OPDs) due to their precisely tunable bandgaps, solution processability, flexibility compatibility, and biocompatibility. However, the narrow‐bandgap intrinsic characteristics required for NIR response inevitably lead to carrier concentration surge that exponentially increases dark current, while hot carriers undergo phonon scattering relaxation that suppresses carrier collection. In this work, the inherent limitations of narrow‐bandgap polymer materials are overcome through a contactless direct current external electric field (EEF). The PTB7‐Th:COTIC‐4F device achieves an outstanding detectivity of 2.45 × 10 13 Jones at 1100 nm, ranking among the highest values reported in the NIR spectral range. The applied EEF modulates both orientation and magnitude of electric dipole moments in acceptors, inducing ordered face‐to‐face molecular stacking, enhancing π–π interactions, and promoting J‐aggregation, thereby facilitating fibrous network formation. Consequently, the optimized film morphology effectively suppresses energetic disorder and electron‐phonon coupling, while simultaneously inhibiting exciton recombination and promoting exciton dissociation to achieve high‐efficiency carrier transport. This non‐contact external field modulation strategy establishes a novel pathway for developing high‐performance NIR‐OPDs.

Article Details

Volume / Issue Vol. 37, Issue 47
Published November 01, 2025
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (12)

X

Xue Shi

J

Jia‐Wei Qiao

School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan Shandong 250100 P. R. China

J

Jin‐Qun Xu

School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan Shandong 250100 P. R. China

P

Peng Lu

The ZeoMat Group, Key Laboratory of Photoelectric Conversion and Utilization of Solar Energy, Qingdao New Energy Shandong Laboratory

H

Hao Wang

Division of Quantitative Sciences, Department of Oncology Johns Hopkins University School of Medicine Baltimore Maryland USA

X

Xin‐Xin Xia

National Engineering Research Center for Colloidal Materials, Key Laboratory of Special Functional Aggregated Materials (Shandong University), Ministry of Education, School of Chemistry & Chemical Engineering Shandong University Jinan Shandong 250100 P. R. China

M

Mao‐Jie Zhang

National Engineering Research Center for Colloidal Materials, Key Laboratory of Special Functional Aggregated Materials (Shandong University), Ministry of Education, School of Chemistry & Chemical Engineering Shandong University Jinan Shandong 250100 P. R. China

K

Kai‐Wen Meng

State Key Lab of Crystal Materials Shandong University Jinan 250100 P. R. China

G

Gang Lian

State Key Laboratory of Crystal Materials Shandong University Jinan P.R. China

X

Xiao‐Yan Du

School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan Shandong 250100 P. R. China

H

Hang Yin

X

Xiao‐Tao Hao

School of Physics State Key Laboratory of Crystal Materials Shandong University Jinan People's Republic of China