Low Threshold, High Q-Factor Optically Pumped Organic Lasers and Exciton Dynamics in OLEDs under High Current Density: Singlet-Triplet Annihilation Effect and toward Electrical Injection Lasing

被引:8
|
作者
Li, Yuanzhao [1 ]
Ying, Shian [2 ]
Zhang, Xiaowei [1 ]
Xiao, Shu [1 ]
Zhang, Dengliang [1 ]
Qiao, Xianfeng [1 ]
Yang, Dezhi [1 ]
Peng, Junbiao [1 ]
Ma, Dongge [1 ]
机构
[1] South China Univ Technol, Ctr Aggregat Induced Emiss Inst Polymer Optoelect, Guangdong Prov Key Lab Luminescence Mol Aggregate, State Key Lab Luminescent Mat & Devices,Guangdong, Guangzhou 510640, Peoples R China
[2] Qingdao Univ Sci & Technol, Key Lab Rubber Plast, Minist Educ, Qingdao 266042, Peoples R China
来源
JOURNAL OF PHYSICAL CHEMISTRY C | 2022年 / 126卷 / 37期
基金
中国国家自然科学基金;
关键词
Current density - Electroluminescence - Excitons - Light - Optically pumped lasers - Organic lasers - Organic light emitting diodes (OLED) - Pumping (laser) - Q factor measurement - Semiconductor lasers;
D O I
10.1021/acs.jpcc.2c04863
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The realization of electrically pumped organic semiconductor lasers needs to suppress singlet-triplet annihilation (STA) as much as possible. Generally, organic gain medium materials suffer extensive loss of singlet excitons through STA, resulting in extremely high lasing threshold current density (J(th)) on the order of 10-100 kA cm(-2). Herein, we study the lasing and electroluminescence (EL) properties of a new organic gain material, named PIO, with low STA. As shown, it exhibits remarkable optical gain and EL performance. A low lasing threshold of 0.47 mJ cm(-2) and a high Q-factor of 6000 are well obtained in the microring resonator. In pulse-driven organic light emitting diodes (OLEDs), a high current density of 112.4 A cm(-2) is achieved. Furthermore, a dynamical model is used to analysis exciton dynamics, gain behaviors and singlet exciton loss channels under electrical excitation. It is found that the rate of STA (k(ST)) is at least lower than 1 x 10(-10) cm(3) s(-1) to realize lasing emission with J(th) below the order of 10 kA cm(-2). The k(ST) of the doped PIO is determined to be 6.6 x 10(-12) cm(3) s(-1). Therefore, it can be predicted that the lasing threshold J(th) of PIO is about 1.20 kA cm(-2).
引用
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页码:16025 / 16033
页数:9
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