Hot exciton dissociation in graphene nanoribbons

G Guanzhao Wen (Max Planck Institute for Polymer Research, Ackermannweg 10, Mainz 55128, Germany) F Fugui Xu (State Key Laboratory of Synergistic Chem-Bio Synthesis, School of Chemistry and Chemical Engineering, Frontiers Science Center for Transformative Molecules, Shanghai Key Laboratory of Electrical Insulation and Thermal Ageing, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China) A Alexander Tries W Wenhao Zheng (Academy for Advanced Interdisciplinary Science and Technology, Beijing Key Laboratory for Advanced Energy Materials and Technologies, State Key Laboratory for Advanced Metals and Materials) L Lucia Di Virgilio S Shuai Fu (Center for Advancing Electronics Dresden and Faculty of Chemistry and Food Chemistry) X Xinyu Chen L Lin Yang Z Zijie Xiao M Mathias Kläui (Institute of Physics, Johannes Gutenberg-University Mainz, Mainz, Germany.) S Silvio Osella (Chemical and Biological Systems Simulation Lab, Centre of New Technologies) J Ji Ma (College of Materials Science and Optoelectronic Technology) X Xu Wang X Xinliang Feng Y Yiyong Mai (State Key Laboratory of Synergistic Chem-Bio Synthesis, School of Chemistry and Chemical Engineering, Frontiers Science Center for Transformative Molecules, Shanghai Key Laboratory of Electrical Insulation and Thermal Ageing, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China) M Mischa Bonn H Hai I. Wang (Max Planck Institute for Polymer Research, Ackermannweg 10, Mainz 55128, Germany)

Abstract

Abstract Exciton dissociation in semiconducting nanostructures is crucial for optoelectronic applications, especially when free-carrier generation is required. Despite considerable research, the question of whether and how such generation occurs in strongly excitonic systems remains elusive. Here, we use one-dimensional precision graphene nanoribbons (GNRs) as a model system to investigate exciton dissociation. We systematically explore the interplay between ribbon length ( l ), excitation energy, and band dispersion in various precision GNRs. Ultrafast Terahertz conductivity measurements reveal that hot exciton dissociation dominates carrier generation, with ribbon length significantly influencing free carrier lifetimes. We identify a critical Bjerrum length ( R B ) of approximately 20 nm that determines whether photoexcited hot carriers in GNRs can dissociate before forming tightly bound excitons. For shorter ribbons ( l  < 2 R B ), rapid ~ps exciton formation prevails. Furthermore, the charge-carrier band dispersion in GNRs plays a critical role in determining dissociation efficiency. Long GNRs with strongly dispersed bands, and consequently low effective carrier masses, exhibit higher mobilities that promote efficient hot-exciton dissociation. These results advance fundamental understanding of dimensionality, energetics, and electronic structure in excitonic materials, providing design principles for optoelectronic devices based on excitonic materials.

Article Details

Volume / Issue Vol. 17, Issue 1
Published June 12, 2026
ISSN 2041-1723
Publisher Nature Portfolio

Journal Info

Nature Communications

Nature Portfolio

ISSN: 2041-1723 Open Access Life Sciences

Authors (17)

G

Guanzhao Wen

Max Planck Institute for Polymer Research, Ackermannweg 10, Mainz 55128, Germany

F

Fugui Xu

State Key Laboratory of Synergistic Chem-Bio Synthesis, School of Chemistry and Chemical Engineering, Frontiers Science Center for Transformative Molecules, Shanghai Key Laboratory of Electrical Insulation and Thermal Ageing, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China

A

Alexander Tries

W

Wenhao Zheng

Academy for Advanced Interdisciplinary Science and Technology, Beijing Key Laboratory for Advanced Energy Materials and Technologies, State Key Laboratory for Advanced Metals and Materials

L

Lucia Di Virgilio

S

Shuai Fu

Center for Advancing Electronics Dresden and Faculty of Chemistry and Food Chemistry

X

Xinyu Chen

L

Lin Yang

Z

Zijie Xiao

M

Mathias Kläui

Institute of Physics, Johannes Gutenberg-University Mainz, Mainz, Germany.

S

Silvio Osella

Chemical and Biological Systems Simulation Lab, Centre of New Technologies

J

Ji Ma

College of Materials Science and Optoelectronic Technology

X

Xu Wang

X

Xinliang Feng

Y

Yiyong Mai

State Key Laboratory of Synergistic Chem-Bio Synthesis, School of Chemistry and Chemical Engineering, Frontiers Science Center for Transformative Molecules, Shanghai Key Laboratory of Electrical Insulation and Thermal Ageing, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China

M

Mischa Bonn

H

Hai I. Wang

Max Planck Institute for Polymer Research, Ackermannweg 10, Mainz 55128, Germany