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Su L. Room temperature amplified spontaneous emissions in a sub-centimeter sized CsPbBr 3 bulk single crystal. OPTICS EXPRESS 2023; 31:39020-39029. [PMID: 38017991 DOI: 10.1364/oe.506043] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/15/2023] [Accepted: 10/10/2023] [Indexed: 11/30/2023]
Abstract
All inorganic perovskite CsPbBr3 shows great potential in laser device because of its excellent luminescence characteristics, while the room temperature amplified spontaneous emission (ASE) in a large size CsPbBr3 bulk single crystal is still quite difficult. Herein, we have obtained the room temperature ASE in a sub-centimeter size CsPbBr3 bulk single crystal pumped with the single-photon excitation. Based on the reproducible light path within the CsPbBr3 bulk single crystal, the photonic feedback between the bottom and top facets naturally enhances the population inversion, which exhibits an amplified spontaneous emission threshold of ∼320 µJ/cm2. The blue shift of the ASE peak along with the increased pumping intensity is also observed and ascribed to the reduction of the refractive index and the energy band filling effect. These findings demonstrate the sub-centimeter size CsPbBr3 bulk single crystal to be an excellent candidate as an optical gain media for crystal lasers.
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Yao X, Wang Y, Wang L, Wang X, Bao Y. The Dissociation of Exciton During the Lasing of a Single CsPbBr 3 Microplate. J Phys Chem Lett 2022; 13:10851-10857. [PMID: 36382934 DOI: 10.1021/acs.jpclett.2c03242] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 06/16/2023]
Abstract
In this work, the lasing of a single CsPbBr3 microplate (MP) fabricated with chemical vapor deposition (CVD) is investigated from the viewpoint of exciton dissociation characterized with steady-state photoluminescence (PL) and time-resolved photoluminescence (TRPL). It is confirmed that the lasing performance is disturbed by the dissociation of excitons. The increase of lasing threshold with temperature originates from the dissociation of free excitons (FEs) to localized carriers (LCs), and the lasing failure is mostly ascribed to the dissociation of FEs to free carriers (FCs). The working temperature of micro/nanolasers based on metal halide perovskites (MHPs) could be raised up to the temperature determined by exciton binding energy while the laser heating effect is dealt with well. These findings advance our understanding on the photophysics of the lasing behaviors of micro/nanocavities based on MHPs and help us promote their performance by having better thermal management.
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Affiliation(s)
- Xiuru Yao
- State Key Laboratory of Superhard Materials & School of Physics, Jilin University, Changchun130012, China
| | - Yu Wang
- State Key Laboratory of Superhard Materials & School of Physics, Jilin University, Changchun130012, China
| | - Lu Wang
- State Key Laboratory of Superhard Materials & School of Physics, Jilin University, Changchun130012, China
| | - Xin Wang
- State Key Laboratory of Superhard Materials & School of Physics, Jilin University, Changchun130012, China
| | - Yongjun Bao
- State Key Laboratory of Superhard Materials & School of Physics, Jilin University, Changchun130012, China
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Shang Q, Li M, Zhao L, Chen D, Zhang S, Chen S, Gao P, Shen C, Xing J, Xing G, Shen B, Liu X, Zhang Q. Role of the Exciton-Polariton in a Continuous-Wave Optically Pumped CsPbBr 3 Perovskite Laser. NANO LETTERS 2020; 20:6636-6643. [PMID: 32786951 DOI: 10.1021/acs.nanolett.0c02462] [Citation(s) in RCA: 59] [Impact Index Per Article: 14.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/22/2023]
Abstract
Lead halide perovskites have emerged as excellent optical gain materials for solution-processable and flexible lasers. Recently, continuous-wave (CW) optically driven lasing was established in perovskite crystals; however, the mechanism of low-threshold operation is still disputed. In this study, CW-pumped lasing from one-dimensional CsPbBr3 nanoribbons (NBs) with a threshold of ∼130 W cm-2 is demonstrated, which can be ascribed to the large refractive index induced by the exciton-polariton (EP) effect. Increasing the temperature reduces the exciton fraction of EPs, which decreases the group and phase refractive indices and inhibits lasing above 100 K. Thermal management, including reducing the NB height to ∼120 ± 60 nm and adopting a high-thermal-conductivity sink, e.g., sapphire, is critical for CW-driven lasing, even at cryogenic temperatures. These results reveal the nature of ultralow-threshold lasing with CsPbBr3 and provide insights into the construction of room-temperature CW and electrically driven perovskite macro/microlasers.
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Affiliation(s)
- Qiuyu Shang
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
| | - Meili Li
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
| | - Liyun Zhao
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
| | - Dingwei Chen
- State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
| | - Shuai Zhang
- CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center of Excellence for Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, China
| | - Shulin Chen
- School of Physics, Peking University, Beijing 100871, China
- Electron Microscopy Laboratory, International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Peng Gao
- School of Physics, Peking University, Beijing 100871, China
- Electron Microscopy Laboratory, International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Chao Shen
- State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
| | - Jun Xing
- Key Laboratory of Eco-Chemical Engineering, Ministry of Education, College of Chemistry and Molecular Engineering, Qingdao University of Science and Technology, Qingdao 266042, China
| | - Guichuan Xing
- Joint Key Laboratory of the Ministry of Education, Institute of Applied Physics and Materials Engineering, University of Macau, Avenida da Universidade Taipa, Macao 999078, China
| | - Bo Shen
- School of Physics, Peking University, Beijing 100871, China
- Research Center for Wide Gap Semiconductor, Peking University, Beijing 100871, China
| | - Xinfeng Liu
- CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center of Excellence for Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, China
| | - Qing Zhang
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
- Research Center for Wide Gap Semiconductor, Peking University, Beijing 100871, China
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