CLC number: TN29
On-line Access: 2021-03-08
Received: 2020-01-17
Revision Accepted: 2020-05-07
Crosschecked: 2020-06-05
Cited: 0
Clicked: 4253
Citations: Bibtex RefMan EndNote GB/T7714
Shuai Wang, Lei Li, Yu-feng Song, Ding-yuan Tang, De-yuan Shen, Lu-ming Zhao. Vector soliton and noise-like pulse generation using a Ti3C2 MXene material in a fiber laser[J]. Frontiers of Information Technology & Electronic Engineering,in press.https://doi.org/10.1631/FITEE.2000033 @article{title="Vector soliton and noise-like pulse generation using a Ti3C2 MXene material in a fiber laser", %0 Journal Article TY - JOUR
在光纤激光器中利用Ti3C2 MXene材料产生矢量孤子和类噪声脉冲1江苏师范大学物理与电子工程学院,江苏省先进激光技术与新兴产业协同创新中心江苏省先进激光材料与器件重点实验室,中国徐州市,221116 2深圳大学深圳市黑磷工程实验室,国际微尺度光电子研究所,教育部二维材料光电科技国际合作联合实验室,中国深圳市,518060 3南洋理工大学电气与电子工程学院,新加坡,639798 4昆山瞬刻激光科技有限公司,中国苏州市,215300 摘要:本文利用Ti3C2 MXene材料作为可饱和吸收体,搭建了铥钬共掺光纤激光器,观察到矢量孤子和类噪声脉冲的形成。其中,可饱和吸收体是通过将Ti3C2溶液滴在侧面抛光的D形光纤上自然挥发后制备而成。观察到的矢量孤子光谱上同时存在两组Kelly边带。通过调节光纤激光器中的偏振控制器,可以将矢量孤子转变为光谱带宽约3.3 nm的类噪声脉冲。据我们所知,这是首次利用Ti3C2 MXene材料作为可饱和吸收体从光纤激光器中获得矢量孤子。 关键词组: Darkslateblue:Affiliate; Royal Blue:Author; Turquoise:Article
Reference[1]Chen Y, Jiang GB, Chen SQ, et al., 2015. Mechanically exfoliated black phosphorus as a new saturable absorber for both Q-switching and mode-locking laser operation. Opt Expr, 23(10):12823-12833. [2]Feng XY, Ding BY, Liang WY, et al., 2018. MXene Ti3C2Tx absorber for a 1.06 μm passively Q-switched ceramic laser. Laser Phys Lett, 15(8):085805. [3]Hantanasirisakul K, Zhao MQ, Urbankowski P, et al., 2016. Fabrication of Ti3C2Tx MXene transparent thin films with tunable optoelectronic properties. Adv Electron Mater, 2(6):1600050. [4]Jiang Q, Zhang M, Zhang Q, et al., 2019. Thulium-doped mode-locked fiber laser with MXene saturable absorber. Conf on Lasers and Electro-Optics, Article SF3O.3. [5]Jiang T, Yin K, Wang C, et al., 2020. Ultrafast fiber lasers mode-locked by two-dimensional materials: review and prospect. Photon Res, 8(1):78-90. [6]Lei JC, Zhang X, Zhou Z, 2015. Recent advances in MXene: preparation, properties, and applications. Front Phys, 10(3):276-286. [7]Li J, Zhang ZL, Du L, et al., 2019. Highly stable femtosecond pulse generation from a MXene Ti3C2Tx (T=F, O, or OH) mode-locked fiber laser. Photon Res, 7(3):260-264. [8]Lu J, Zou X, Li C, et al., 2017. Picosecond pulse generation in a mono-layer MoS2 mode-locked Ytterbium-doped thin disk laser. Chin Opt Lett, 15(4):041401. [9]Luo ZQ, Zhou M, Weng J, et al., 2010. Graphene-based passively Q-switched dual-wavelength erbium-doped fiber laser. Opt Lett, 35(21):3709-3711. [10]Miao RL, Tong MY, Yin K, et al., 2019. Soliton mode-locked fiber laser with high-quality MBE-grown Bi2Se3 film. Chin Opt Lett, 17(7):071403. [11]Naguib M, Kurtoglu M, Presser V, et al., 2011. Two‐ dimensional nanocrystals produced by exfoliation of Ti3AlC2. Adv Mater, 23(37):4248-4253. [12]Nicholson JW, Windeler RS, DiGiovanni DJ, 2007. Optically driven deposition of single-walled carbon-nanotube saturable absorbers on optical fiber end-faces. Opt Expr, 15(15):9176-9183. [13]Qin ZP, Xie GQ, Zhang H, et al., 2015. Black phosphorus as saturable absorber for the Q-switched Er:ZBLAN fiber laser at 2.8 μm. Opt Expr, 23(19):24713-24718. [14]Scholle K, Lamrini S, Koopmann P, et al., 2010. 2 µm laser sources and their possible applications. In: Pal B (Ed.), Frontiers in Guided Wave Optics and Optoelectronics. InTech, Vukovar, p.471-500. [15]Shi W, Fang Q, Zhu XS, et al., 2014. Fiber lasers and their applications [invited]. Appl Opt, 53(28):6554-6568. [16]Song YF, Zhang H, Tang DY, et al., 2012. Polarization rotation vector solitons in a graphene mode-locked fiber laser. Opt Expr, 20(24):27283-27289. [17]Song YF, Chen S, Zhang Q, et al., 2016. Vector soliton fiber laser passively mode locked by few layer black phosphorus-based optical saturable absorber. Opt Expr, 24(23):25933-25942. [18]Song YF, Chen YX, Jiang XT, et al., 2019a. Nonlinear few‐layer MXene‐assisted all‐optical wavelength conversion at telecommunication band. Adv Opt Mater, 7(18):1801777. [19]Song YF, Shi XJ, Wu CF, et al., 2019b. Recent progress of study on optical solitons in fiber lasers. Appl Phys Rev, 6(2):021313. [20]Sotor J, Sobon G, Kowalczyk M, et al., 2015. Ultrafast thulium-doped fiber laser mode locked with black phosphorus. Opt Lett, 40(16):3885-3888. [21]Tang YX, Chong A, Wise FW, 2015. Generation of 8 nJ pulses from a normal-dispersion thulium fiber laser. Opt Lett, 40(10):2361-2364. [22]Wang C, Peng QQ, Fan XW, et al., 2018. MXene Ti3C2Tx saturable absorber for pulsed laser at 1.3 μm. Chin Phys B, 27(9):094214. [23]Wang C, Wang YZ, Jiang XT, et al., 2019. MXene Ti3C2Tx: a promising photothermal conversion material and application in all‐optical modulation and all‐optical information loading. Adv Opt Mater, 7(12):1900060. [24]Yin K, Zhang B, Li L, et al., 2015. Soliton mode-locked fiber laser based on topological insulator Bi2Te3 nanosheets at 2 μm. Photon Res, 3(3):72-76. [25]Zhang CX, Ouyang H, Miao RL, et al., 2019. Anisotropic nonlinear optical properties of a SnSe flake and a novel perspective for the application of all‐optical switching. Adv Opt Mater, 7(18):1900631. [26]Zhang H, Tang DY, Zhao LM, et al., 2009. Large energy mode locking of an erbium-doped fiber laser with atomic layer graphene. Opt Expr, 17(20):17630-17635. [27]Zhang H, Tang DY, Knize RJ, et al., 2010. Graphene mode locked, wavelength-tunable, dissipative soliton fiber laser. Appl Phys Lett, 96(11):111112. [28]Zhang J, Jiang T, Zhou T, et al., 2018. Saturated absorption of different layered Bi2Se3 films in the resonance zone. Photon Res, 6(10):C8-C14. [29]Zhao B, Tang DY, Kong J, et al., 2005. Periodic soliton amplitude variation caused by unstable dispersive waves in a laser. Opt Commun, 254(4-6):242-247. [30]Zu YQ, Zhang C, Guo XS, et al., 2019. A solid-state passively Q-switched Tm,Gd:CaF2 laser with a Ti3C2Tx MXene absorber near 2 µm. Laser Phys Lett, 16(1):015803. Journal of Zhejiang University-SCIENCE, 38 Zheda Road, Hangzhou
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