Engineering Edge States of Graphene Nanoribbons for Narrow-Band PhotoluminescenceClick to copy article linkArticle link copied!
- Chuanxu MaChuanxu MaCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesDepartment of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, United StatesHefei National Research Center for Physical Sciences at the Microscale and Synergetic Innovation Center of Quantum Information & Quantum Physics, University of Science and Technology of China, Hefei, Anhui 230026, ChinaMore by Chuanxu Ma
- Zhongcan XiaoZhongcan XiaoDepartment of Physics, North Carolina State University, Raleigh, North Carolina 27695, United StatesMore by Zhongcan Xiao
- Alexander A. PuretzkyAlexander A. PuretzkyCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Alexander A. Puretzky
- Hao WangHao WangDepartment of Electrical Engineering and Computer Science, University of Tennessee, Knoxville, Tennessee 37996, United StatesMore by Hao Wang
- Ali MohsinAli MohsinDepartment of Electrical Engineering and Computer Science, University of Tennessee, Knoxville, Tennessee 37996, United StatesMore by Ali Mohsin
- Jingsong HuangJingsong HuangCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesComputational Sciences and Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Jingsong Huang
- Liangbo LiangLiangbo LiangCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Liangbo Liang
- Yingdong LuoYingdong LuoCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Yingdong Luo
- Benjamin J. LawrieBenjamin J. LawrieCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Benjamin J. Lawrie
- Gong GuGong GuDepartment of Electrical Engineering and Computer Science, University of Tennessee, Knoxville, Tennessee 37996, United StatesMore by Gong Gu
- Wenchang LuWenchang LuDepartment of Physics, North Carolina State University, Raleigh, North Carolina 27695, United StatesComputational Sciences and Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Wenchang Lu
- Kunlun HongKunlun HongCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Kunlun Hong
- Jerzy BernholcJerzy BernholcDepartment of Physics, North Carolina State University, Raleigh, North Carolina 27695, United StatesComputational Sciences and Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Jerzy Bernholc
- An-Ping Li*An-Ping Li*Email: [email protected]Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesDepartment of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, United StatesMore by An-Ping Li
Abstract
Solid-state narrow-band light emitters are on-demand for quantum optoelectronics. Current approaches based on defect engineering in low-dimensional materials usually introduce a broad range of emission centers. Here, we report narrow-band light emission from covalent heterostructures fused to the edges of graphene nanoribbons (GNRs) by controllable on-surface reactions from molecular precursors. Two types of heterojunction (HJ) states are realized by sequentially synthesizing GNRs and graphene nanodots (GNDs) and then coupling them together. HJs between armchair GNDs and armchair edges of the GNR are coherent and give rise to narrow-band photoluminescence. In contrast, HJs between the armchair GNDs and the zigzag ends of GNRs are defective and give rise to nonradiative states near the Fermi level. At low temperatures, sharp photoluminescence emissions with peak energy range from 2.03 to 2.08 eV and line widths of 2–5 meV are observed. The radiative HJ states are uniform, and the optical transition energy is controlled by the band gaps of GNRs and GNDs. As these HJs can be synthesized in a large quantity with atomic precision, this finding highlights a route to programmable and deterministic creation of quantum light emitters.
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