Hot exciton dissociation in graphene nanoribbons
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
Authors (17)
Guanzhao Wen
Max Planck Institute for Polymer Research, Ackermannweg 10, Mainz 55128, Germany
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
Alexander Tries
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
Lucia Di Virgilio
Shuai Fu
Center for Advancing Electronics Dresden and Faculty of Chemistry and Food Chemistry
Xinyu Chen
Lin Yang
Zijie Xiao
Mathias Kläui
Institute of Physics, Johannes Gutenberg-University Mainz, Mainz, Germany.
Silvio Osella
Chemical and Biological Systems Simulation Lab, Centre of New Technologies
Ji Ma
College of Materials Science and Optoelectronic Technology
Xu Wang
Xinliang Feng
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
Mischa Bonn
Hai I. Wang
Max Planck Institute for Polymer Research, Ackermannweg 10, Mainz 55128, Germany