Two‐Stage Bipolaron Formation in Molecularly Doped Conjugated Polymers

R Rui Su J Jingshan Chai Y Yusen Pei (Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA) Y Yusuf Olanrewaju (Department of Materials Science and Engineering) L Liang Yan (Department of Chemistry) J Justin Neu (Department of Chemistry) J Jake Mauthe (Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA) K Katherine Stewart (Department of Physics and Centre for Processable Electronics Imperial College London Blackett Laboratory London SW7 2AZ UK) S Somayeh Kashani (Department of Physics and Organic and Carbon Electronics Laboratories (ORaCEL)) N Neha Chaturvedi (Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA) S Stefan Nikodemski (KBR Inc. 3 , Beavercreek, Ohio 45431,) J Jarrett H. Vella (Sensors Directorate Air Force Research Laboratory Wright‐Patterson Air Force Base (AFB) Dayton OH 45433 USA) A Aram Amassian (Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA) D David S. Ginger (Department of Chemistry) J Ji‐Seon Kim (Department of Physics and Centre for Processable Electronics Imperial College London Blackett Laboratory London SW7 2AZ UK) H Harald Ade (Department of Physics and Organic and Carbon Electronics Laboratories (ORaCEL)) W Wei You (Department of Polymer Science and Engineering) F Franky So

Abstract

Abstract The formation and dynamics of bipolarons are crucial in determining the electrical properties of molecularly doped conjugated polymers. Traditionally, bipolarons are known to form at very high doping levels through the combination of two adjacent polarons, a process that is generally accompanied by structural disorder and impaired carrier transport. Here, it is demonstrated that bipolaron formation can occur at both the early stage with low doping levels and the late stage with high doping levels in 2,3,5,6‐tetrafluoro‐7,7,8,8‐tetracyanoquinodimethane (F 4 TCNQ) dip‐doped conjugated polymer films with glycol sidechains. Bipolaron formation at the early stage is discovered to be mainly associated with double doping, which is uncommon in conventional doped polymer systems. In contrast, bipolaron formation at the late stage is dominated by combining two polarons. Furthermore, these bipolarons are observed to behave differently: early‐stage bipolarons generated through double doping enhance both the molecular ordering and carrier transport, whereas late‐stage bipolarons resulting from polaron combination occur alongside detrimental effects in structural and transport properties. These findings provide new insights into the mechanisms of bipolaron formation across different doping levels and underscore the potential for optimizing doping strategies. A deeper understanding of bipolarons can guide the design of next‐generation molecularly doped conjugated polymers with improved performance.

Article Details

Volume / Issue Vol. 37, Issue 42
Published October 01, 2025
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (18)

R

Rui Su

J

Jingshan Chai

Y

Yusen Pei

Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA

Y

Yusuf Olanrewaju

Department of Materials Science and Engineering

L

Liang Yan

Department of Chemistry

J

Justin Neu

Department of Chemistry

J

Jake Mauthe

Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA

K

Katherine Stewart

Department of Physics and Centre for Processable Electronics Imperial College London Blackett Laboratory London SW7 2AZ UK

S

Somayeh Kashani

Department of Physics and Organic and Carbon Electronics Laboratories (ORaCEL)

N

Neha Chaturvedi

Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA

S

Stefan Nikodemski

KBR Inc. 3 , Beavercreek, Ohio 45431,

J

Jarrett H. Vella

Sensors Directorate Air Force Research Laboratory Wright‐Patterson Air Force Base (AFB) Dayton OH 45433 USA

A

Aram Amassian

Department of Materials Science and Engineering North Carolina State University Raleigh NC 27695 USA

D

David S. Ginger

Department of Chemistry

J

Ji‐Seon Kim

Department of Physics and Centre for Processable Electronics Imperial College London Blackett Laboratory London SW7 2AZ UK

H

Harald Ade

Department of Physics and Organic and Carbon Electronics Laboratories (ORaCEL)

W

Wei You

Department of Polymer Science and Engineering

F

Franky So