Author Affiliations
Abstract
1 School of Information Science and Engineering, Shandong University, Qingdao 266237, China
2 School of Physics and Technology, University of Jinan, Jinan 250022, China
We report VOx/NaVO3 nanocomposite as a novel saturable absorber for the first time, to the best of our knowledge. The efficient nonlinear absorption coefficient and the modulation depth are determined by the Z-scan technology. As a saturable absorber, a passively Q-switched Nd-doped bulk laser at 1.34 µm is demonstrated, producing the shortest pulse duration of 129 ns at a repetition rate of 274 kHz. In the passively Q-switched Tm:YLF laser with the prepared saturable absorber, the shortest pulse duration was 292 ns with a repetition rate of 155 kHz. Our work confirmed the saturable absorption in VOx/NaVO3 for possible optical modulation in the near-infrared region.
nonlinear optical properties saturable absorber VOx/NaVO3 composite Q-switching 
Chinese Optics Letters
2022, 20(5): 051601
作者单位
摘要
中国激光
2021, 48(12): 1200000
作者单位
摘要
1 山东大学信息科学与工程学院, 山东 青岛 266237
2 山东大学晶体材料研究所, 山东 济南 250100
时至今日,非线性光学材料在光电子、通信、信息处理等领域的重要作用日益突出,发展新型、优良的非线性光学材料迫在眉睫。与传统的无机非线性光学材料相比,有机非线性光学材料在损伤阈值、响应时间和非线性光学系数上具有决定性优势。沸石咪唑酯骨架结构材料(ZIFs)是一类以咪唑或其衍生物为配体的特殊金属有机骨架结构材料,其以结构多样性、高度的热学和化学稳定性,近年来受到了国内外研究者的关注。本文总结了沸石咪唑酯骨架结构材料制备方法以及非线性光学特性的研究进展,并就沸石咪唑酯骨架结构材料在非线性光学领域的应用前景进行了展望。
材料 非线性光学材料 纳米材料 金属有机纳米骨架 沸石咪唑酯骨架结构 调Q 
中国激光
2021, 48(12): 1203001
作者单位
摘要
山东大学信息科学与工程学院, 山东 青岛 266237
自石墨烯发现以来,新型单元素纳米材料以其新奇的光电特性备受关注。特别是近几年来,第五主族元素纳米材料(砷烯、锑烯、铋烯)更是激发了研究人员的极大兴趣。作为一种过渡金属,铋纳米材料一直是材料和光学研究领域的热点之一,在电子器件、光电器件和非线性光学等领域的应用中表现出巨大的潜力和良好的前景。首先,着重从制备、表征和非线性光学特性研究等方面介绍铋纳米材料的相关理论和实验研究工作。接着,总结铋纳米材料的非线性光学性质及其光子学应用规律。最后,对铋纳米材料的发展前景和趋势进行展望和分析。
纳米材料 铋烯 非线性光学性质 锁模 调Q 
中国激光
2021, 48(12): 1208002
Author Affiliations
Abstract
1 School of Information Science and Engineering, and Shandong Provincial Key Laboratory of Laser Technology and Application, Shandong University, Qingdao 266237, China
2 Key Laboratory of Colloid and Interface Chemistry, Ministry of Education, School of Chemistry and Chemical Engineering, Shandong University, Jinan 250100, China
Gold nanorods (GNRs) with two different aspect ratios were successfully utilized as saturable absorbers (SAs) in a passively Q-switched neodymium-doped lutetium lithium fluoride (Nd:LLF) laser emitting at 1.34 μm. Based on the GNRs with an aspect ratio of five, a maximum output power of 1.432 W was achieved, and the narrowest pulse width was 328 ns with a repetition rate of 200 kHz. But, in the case of the GNRs with the aspect ratio of eight, a maximum output power of 1.247 W was achieved, and the narrowest pulse width was 271 ns with a repetition rate of 218 kHz. Our experimental results reveal that the aspect ratios of GNRs have different saturable absorption effects at a specific wavelength. In other words, for passively Q-switched lasers at a given wavelength, we are able to select the most suitable GNRs as an SA by changing their aspect ratio.
140.3480 Lasers, diode-pumped 140.3540 Lasers, Q-switched 140.3070 Infrared and far-infrared lasers 
Chinese Optics Letters
2019, 17(4): 041401
Author Affiliations
Abstract
1 School of Information Science and Engineering, Shandong University, Jinan 250100, China
2 Department of Photonics, Taiwan Sun Yat-sen University, 70 Lienhei Road, Kaohsiung 80424, China
3 State Key Laboratory of Crystal Materials, Institute of Crystal Materials, Shandong University, Jinan 250100, China
4 Research Center for Applied Sciences, Academia Sinica, 128 Sec. 2, Academic Road, Taipei 11529, China
5 e-mail: shengzhi_zhao@sdu.edu.cn
6 e-mail: chuckcklee@yahoo.com
In this paper, the fabrication process and characterization of Bi2Te3 topological insulators (TIs) synthesized by the spin-coating-coreduction approach (SCCA) is reported. With this approach, high-uniformity nano-crystalline TI saturable absorbers (TISAs) with large-area uniformity and controllable thickness are prepared. By employing these prepared TIs with different thicknesses as SAs in 2-μm solid-state Q-switched lasers, thickness-dependent output powers and pulse durations of the laser pulses are obtained, and the result also exhibits stability and reliability. The shortest pulse duration is as short as 233 ns, and the corresponding clock amplitude jitter is around 2.1%, which is the shortest pulse duration in TISA-based Q-switched 2-μm lasers to the best of our knowledge. Moreover, in comparison with the TISA synthesized by the ultrasound-assisted liquid phase exfoliation (UALPE) method, the experimental results show that lasers with SCCA synthesized TISAs have higher output powers, shorter pulse durations, and higher pulse peak powers. Our work suggests that the SCCA synthesized TISAs could be used as potential SAs in pulsed lasers.
Lasers, Q-switched Optical properties 
Photonics Research
2018, 6(4): 04000314
Author Affiliations
Abstract
School of Information Science and Engineering, Shandong University, 27 Shanda South Road, Jinan 250100, China
By simultaneously employing both an electro-optic modulator and carbon nanotube saturable absorber (CNT-SA) in a dual-loss modulator, a subnanosecond single mode-locking pulse underneath a Q-switched envelope with high peak power was generated from a doubly Q-switched and mode-locked (QML) Nd:Lu0.15Y0.85VO4 laser at 1.06 μm for the first time, to our knowledge. CNTs with different wall structures—single-walled CNTs (SWCNTs), double-walled CNTs (DWCNTs), and multi-walled CNTs (MWCNTs)—were used as SAs in the experiment to investigate the single mode-locking pulse characteristics. At pump power of 10.72 W, the maximum peak power of 1.312 MW was obtained with the DWCNT.
Lasers Lasers frequency modulated frequency modulated Lasers Lasers pulsed pulsed Lasers Lasers solid-state solid-state Mode-locked lasers Mode-locked lasers 
Photonics Research
2017, 5(1): 01000046
Author Affiliations
Abstract
1 School of Information Science and Engineering, and Shandong Provincial Key Laboratory of Laser Technology and Application, Shandong University, Jinan 250100, China
2 Key Laboratory of Colloid and Interface Chemistry of State Education Ministry, School of Chemistry and Chemical Engineering, Shandong University, Jinan 250100, China
3 Institut für Laser-Physik, Universit?t Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany
4 Hamburg Centre for Ultrafast Imaging, Universit?t Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany
5 e-mail: kraenkel@physnet.uni?hamburg.de
Multilayer black phosphorus (BP) nanoplatelets of different thicknesses were prepared by the liquid phase exfoliation method and deposited onto yttrium aluminum garnet substrates to form saturable absorbers (SAs). These were characterized with respect to their thickness-dependent saturable absorption properties at 3 μm. The BP-SAs were employed in a passively Q-switched Er:Lu2O3 laser at 2.84 μm. By using BP exfoliated in different solvents, stable pulses as short as 359 ns were generated at an average output power of up to 755 mW. The repetition rate in the experiment was 107 kHz, corresponding to a pulse energy of 7.1 μJ. These results prove that BP-SAs have a great potential for optical modulation in the mid-infrared range.
Laser materials Laser materials Infrared and far-infrared lasers Infrared and far-infrared lasers Lasers Lasers Q-switched Q-switched 
Photonics Research
2016, 4(5): 05000181
Author Affiliations
Abstract
School of Information Science and Engineering, Shandong University, Jinan 250100, China
A Kerr-lens, mode-locked YVO4∕Nd:YVO4 laser coupled with an acousto-optic modulator (AOM) Q-switching near 1064 nm was employed to pump an intracavity KTiOPO4 (KTP) optical parametric oscillator. A subnanosecond signal wave near 1572 nm with low repetition rate was realized. At an AOM repetition rate of 8 kHz, the maximum output power was 165 mW. The highest average pulse energy, the shortest duration, and the highest peak power of a mode-locking signal pulse were estimated to be ~10.3 μJ, ~120 ps, and ~82 kW, respectively.
Nonlinear optics Nonlinear optics parametric processes parametric processes Ultrafast lasers Ultrafast lasers Kerr effect Kerr effect 
Photonics Research
2015, 3(5): 05000260

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