Realizing Near-Infrared Laser Dyes through a Shift in Excited-State Absorption

被引:32
|
作者
Aoki, Reiko [1 ,2 ]
Komatsu, Ryutaro [1 ,2 ,3 ]
Goushi, Kenichi [1 ,2 ]
Mamada, Masashi [1 ,2 ]
Ko, Soo Young [4 ]
Wu, Jeong Weon [5 ]
Placide, Virginie [5 ]
D'Aleo, Anthony [6 ]
Adachi, Chihaya [1 ,2 ,7 ]
机构
[1] Kyushu Univ, Ctr Organ Photon & Elect Res OPERA, Fukuoka 8190395, Japan
[2] Kyushu Univ, Ctr Organ Photon & Elect Res OPERA, Adachi Mol Exciton Engn Project, JST ERATO,Nishi Ku, Fukuoka 8190395, Japan
[3] KOALA Tech Inc, 3-5-12 Fukuoka Ind Acad Symphonicity FiaS, Fukuoka 8190388, Japan
[4] Ewha Womans Univ, Dept Chem, Seoul, South Korea
[5] Ewha Womans Univ, Dept Phys, Seoul 03760, South Korea
[6] Yonsei Univ, Sorbonne Univ, CNRS, Bldg Blocks Future Elect Lab,UMI 2002, 50 Yonsei Ro, Seoul 03722, South Korea
[7] Kyushu Univ, Int Inst Carbon Neutral Energy Res WPI I2CNER, Nishi Ku, Nishi, Fukuoka 8190395, Japan
关键词
amplified spontaneous emission; distributed feedback laser; organic light-emitting diodes; organic semiconductor laser diodes; thermally activated delayed fluorescence; AMPLIFIED SPONTANEOUS EMISSION; ELECTROLUMINESCENCE;
D O I
10.1002/adom.202001947
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The development of near-infrared (NIR) light sources has attracted much interest due to their attractive applications, such as biosensing and light detection and ranging (LiDAR). In particular, organic semiconductor laser diodes with NIR emission are emerging as a next generation technology. However, organic NIR emitters have generally suffered from a low quantum yield, which has resulted in only a few examples of organic solid-state NIR lasers. In this study, the authors demonstrate a highly efficient NIR emitter based on a boron difluoride curcuminoid structure, which shows a high photoluminescence (PL) quantum yield (phi(PL)) at >700 nm and a high fluorescence radiative rate constant in a solid-state film. Amplified spontaneous emission and lasing occurs at >800 nm with very low thresholds. The large redshift of the stimulated emission is attributed to the transition from the lowest excited state to the different vibrational levels of the ground state owing to the overlap between the emission and the singlet-singlet excited-state absorption.
引用
收藏
页数:6
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