Research progress of pure quartic soliton fiber laser

Luo Min; Zhang Ze-Xian; Chen Nai-Miao; Liu Meng; Luo Ai-Ping; Xu Wen-Cheng; Luo Zhi-Chao

doi:10.7498/aps.72.20230868

Abstract

The pure-quartic soliton fiber laser is an innovative ultra-short pulse laser that can maintain a stable pulse shape through a balance between fourth-order dispersion effect and self-phase modulation effect. Comparing with traditional soliton laser that is dominated by second-order dispersion, the mode-locked pulse energy of pure-quartic soliton laser can be 1–2 orders of magnitude higher. This provides researchers with new ideas for developing high-energy and high-peak-power fiber lasers. Here, the generation and transmission characteristics of pure-quartic solitons in nonlinear optical systems such as fiber lasers in recent years are systematically reviewed. It also explores some special transient dynamic phenomena. Furthermore, in this article, the latest achievements of our research group in this area are also presented. Finally, the application prospect and development trend of pure-quartic soliton fiber lasers are prospected. These results will contribute to a more comprehensive understanding of the basic physical properties of pure-quartic soliton fiber lasers.

Keywords:

Authors and contacts

School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510631, China

Corresponding author: Luo Zhi-Chao, zcluo@scnu.edu.cn

Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. 11874018, 11974006, 61805084, 61875058) and the Natural Science Foundation of Guangdong Province, China (Grant Nos. 2022A1515011760, 2021A1515012315).

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References

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Cited By

图 1 纯四次孤子概念及其及实验证明^[22]　(a) 纯四次孤子原理图; (b) 频率分辨电开关; (c) 扫描电子显微镜下的样品图像; (d) 光子晶体波导的色散测量

Figure 1. Concept of pure-quartic solitons and their experimental demonstration^[22]: (a) Schematic of pure-quartic solitons; (b) frequency-resolved electrical gating; (c) scanning electron microscopy image of the sample; (d) measured dispersion of the photonic crystal waveguides.

DownLoad: Full-Size Img PowerPoint

图 2 不同输入功率下的频域和时域结果(红色虚线为实验结果, 蓝色实线为模拟结果)^[22]

Figure 2. Frequency domain and time domain results at different input powers (the red dashed line is the experimental result, and the solid blue line is the simulation result)^[22].

DownLoad: Full-Size Img PowerPoint

图 3 纯四次孤子输出特性　(a) 线性坐标下的时域脉冲; (b) 对数坐标下的时域脉冲; (c) 线性坐标下的频域光谱; (d) 对数坐标下的频域光谱(红色为常规孤子光谱)^[46]

Figure 3. Output characteristics of pure-quartic solitons: (a) Time domain pulses at linear coordinates; (b) time domain pulses at logarithmic coordinates; (c) frequency domain spectrum in linear coordinates; (d) frequency domain spectrum in logarithmic coordinates (red is the spectrum of traditional soliton)^[46].

DownLoad: Full-Size Img PowerPoint

图 4 纯四次孤子光纤激光器原理示意图　(a) 实验装置图; (b) 二阶色散相位; (c)四阶色散相位^[23]

Figure 4. Schematic diagram of pure-quartic fiber soliton laser: (a) Experimental setup; (b) second-order dispersion phases; (c) fourth-order dispersion phases^[23].

DownLoad: Full-Size Img PowerPoint

图 5 实验和模拟上的光谱和时域曲线　(a)—(d) 传统孤子; (e)—(h) 纯四次孤子^[23]

Figure 5. Experimental (exp.) and simulated (sim.) spectra and time-domain curves: (a)–(d) Conventional solitons; (e)–(h) pure-quartic solitons^[23].

DownLoad: Full-Size Img PowerPoint

图 6 自相似纯四次孤子激光器　(a) 模拟结构图; (b)时域曲线; (c) 频域曲线^[25]

Figure 6. Self-similar pure-quartic soliton laser: (a) Simulation structure diagram; (b) time domain curves; (c) frequency domain curves^[25]

DownLoad: Full-Size Img PowerPoint

图 7 耗散纯四次孤子^[26]　(a) 线性与对数坐标下的光谱; (b) 脉冲和啁啾; (c), (d) 1000圈下的频域和时域演化

Figure 7. Dissipative pure-quartic solitons^[26]: (a) Spectrum with log and linear coordinates; (b) pulse and chirp; (c), (d) evolution of frequency domain and time domain with 1000 roundtrips.

DownLoad: Full-Size Img PowerPoint

图 8 非对称“M”型耗散纯四次孤子^[26]　(a) 线性与对数坐标下的光谱; (b) 脉冲(蓝色)和啁啾(红色); (c), (d) 1000圈下的频域和时域演化

Figure 8. Asymmetric “M” type dissipative pure-quartic solitons^[26]: (a) Spectrum with log and linear coordinates; (b) pulse (blue) and chirp (red); (c), (d) evolution of frequency domain and time domain with 1000 roundtrips.

DownLoad: Full-Size Img PowerPoint

图 9 纯高阶色散孤子六次色散(上行)、八次色散(中行)和十次色散(下行)的频域和时域测量　(a)—(c) 测量光谱(蓝色)和计算光谱(红色虚线); (d)—(f) 频谱图; (g)—(i) 时域强度(蓝色)、相位(橙色)以及相应的计算时域形状(红色虚线)^[48]

Figure 9. Spectral and temporal measurements of pure high-order dispersion solitons sextic (top row), octic (middle row), and decic (bottom row) dispersion: (a)–(c) Measured (blue) and calculated (red-dashed) spectrum; (d)–(f) spectrograms; (g)–(i) temporal intensity (blue), phase (orange), and corresponding calculated temporal shapes (red-dashed)^[48].

DownLoad: Full-Size Img PowerPoint

图 10 纯四次孤子在不同初始相位差条件下碰撞动力学^[49]

Figure 10. Collision dynamics of pure-quartic solitons with different initial phase differences^[49].

DownLoad: Full-Size Img PowerPoint

图 11 纯四次孤子的脉动状态^[50]　(a) 时域的演化(插图为纯四次孤子中心部分(绿色)和振荡尾(白色)的能量演化); (b)光谱域的演化

Figure 11. Pulsation state of pure-quartic solitons^[50]: (a) Evolution of the time domain(energy evolution of the pure quadruple soliton center (green) and oscillating tail (white)); (b) evolution of the spectral domain.

DownLoad: Full-Size Img PowerPoint

图 12 (a) 具有不同饱和能量值的纯四次孤子的归一化峰值强度演化; (b), (c) 不同饱和能量下脉冲的两个典型分布^[50]

Figure 12. (a) Normalized peak intensity evolution of pure-quartic solitons with different saturation energy values; (b), (c) two typical pulse distributions under different saturated energies^[50].

DownLoad: Full-Size Img PowerPoint

图 13 (a) 拉曼效应下纯四次孤子的峰值功率(黑点)与泵浦功率(红色虚线)的关系(呼吸状态由灰色区域显示); (b) 稳定状态(泵浦功率为1 W, 6 W)和 (c) 呼吸状态(泵浦功率为4 W)的时域脉冲及其相应相位(红线); (d) 4 W泵浦功率下拉曼纯四次孤子呼吸的典型频谱; (e) 呼吸状态谱能量演化(白色虚线表示不同段的光谱能量峰值)^[52]

Figure 13. (a)The relationship between peak power (black dot) and pump power (red dashed line) of Raman pure-quartic solitons (the breathing state is shown by the gray area); (b) time domain pulses in stable state (pump powers are 1 W and 6 W) and (c) breathing state (pump power is 4 W) and corresponding phases (red line); (d) typical breathing spectrum of Raman pure-quartic solitons at pump power of 4 W; (e) energy evolution of the breathing spectrum (the white dotted lines indicate the spectral energy peaks in different segments)^[52].

DownLoad: Full-Size Img PowerPoint

[1]	Cundiff S T, Ye J 2003 Rev. Mod. Phys. 75 325 Google Scholar
[2]	Yi X, Yang Q F, Yang K Y, Suh M G, Vahala K 2015 Optica 2 1078 Google Scholar
[3]	Okhotnikov O, Grudinin A, Pessa M 2004 New J. Phys. 6 177 Google Scholar
[4]	Wise F W, Chong A, Renninger W H 2008 Laser Photon. Rev. 2 58 Google Scholar
[5]	Grelu P, Akhmediev N 2012 Nat. Photonics 6 84 Google Scholar
[6]	Xu C, Wise F W 2013 Nat. Photonics 7 875 Google Scholar
[7]	Wang K, Horton N G, Charan K, Xu C 2014 IEEE J. Sel. Top. Quant. 20 50 Google Scholar
[8]	Mollenauer L F, Stolen R H, Gordon J P 1980 Phys. Rev. Lett. 45 1095 Google Scholar
[9]	Agrawal G P 2007 Nonlinear Fiber Optics (4th Ed.) (Academic Press
[10]	Fermann M E, Hartl I 2013 Nat. Photonics 7 868 Google Scholar
[11]	Dennis M L, Duling I N 1994 IEEE J. Quantum Elect. 30 1469 Google Scholar
[12]	Nelson L E, Jones D J, Tamura K, Haus H A, Ippen E P 1997 Appl. Phys. B 65 277 Google Scholar
[13]	Shabat A, Zakharov V 1972 Sov. Phys. JETP 34 62
[14]	Renninger W H, Chong A, Wise F W 2010 J. Opt. Soc. Am. B 27 1978 Google Scholar
[15]	Tamura K, Ippen E P, Haus H A, Nelson L E 1993 Opt. Lett. 18 1080 Google Scholar
[16]	Chong A, Buckley J, Renninger W, Wise F 2006 Opt. Express 14 10095 Google Scholar
[17]	Blow K J, Doran N J, Wood D 1988 J. Opt. Soc. Am. B 5 381 Google Scholar
[18]	Karlsson M, Höök A 1994 Opt. Commun. 104 303 Google Scholar
[19]	Christov I P, Murnane M M, Kapteyn H C, Zhou J, Huang C P 1994 Opt. Lett. 19 1465 Google Scholar
[20]	Piché M, Cormier J F, Zhu X 1996 Opt. Lett. 21 845 Google Scholar
[21]	Roy S, Biancalana F 2013 Phys. Rev. A 87 025801 Google Scholar
[22]	Blanco-Redondo A, de Sterke C M, Sipe J E, Krauss T F, Eggleton B J, Husko C 2016 Nat. Commun. 7 10427 Google Scholar
[23]	Runge A F J, Hudson D D, Tam K K K, de Sterke C M, Blanco-Redondo A 2020 Nat. Photonics 14 492 Google Scholar
[24]	de Sterke C M, Runge A F J, Hudson D D, Blanco-Redondo A 2021 APL Photonics 6 091101 Google Scholar
[25]	Runge A F J, Alexander T J, Newton J, Alavandi P A, de Sterke C M 2020 Opt. Lett. 45 3365 Google Scholar
[26]	Qian Z C, Liu M, Luo A P, Xu W C, Luo Z C 2022 Opt. Express 30 22066 Google Scholar
[27]	Soto-Crespo J M, Akhmediev N, Ankiewicz A 2000 Phys. Rev. Lett. 85 2937 Google Scholar
[28]	Akhmediev N, Soto-Crespo J M, Town G 2001 Phys. Rev. E 63 056602 Google Scholar
[29]	Zhao L M, Tang D Y, Lin F, Zhao B 2004 Opt. Express 12 4573 Google Scholar
[30]	Liu M, Wei Z W, Li H, Li T J, Luo A P, Xu W C, Luo Z C 2020 Laser Photonics Rev. 14 1900317 Google Scholar
[31]	Akhmediev N, Soto-Crespo J M 2003 Phys. Lett. A 317 287 Google Scholar
[32]	Liu M, Luo A P, Yan Y R, Hu S, Liu Y C, Cui H, Luo Z C, Xu W C 2016 Opt. Lett. 41 1181 Google Scholar
[33]	Luo M, Zhang Z X, Liu M, Luo A P, Xu W C, Luo Z C 2022 Opt. Express 30 22143 Google Scholar
[34]	Luo M, Zhang Z X, Chen N M, Liu M, Luo A P, Xu W C, Luo Z C 2023 Adv. Phys. Res. 2 2200103 Google Scholar
[35]	Aossey D W, Skinner S R, Cooney J L, Williams J E, Gavin M T, Andersen D R, Lonngren K E 1992 Phys. Rev. A 45 2606 Google Scholar
[36]	Liu M, Li T J, Luo A P, Xu W C, Luo Z C 2020 Laser Photon. Rev. 14 1900317 Google Scholar
[37]	Wai P K A, Chen H H, Lee Y C 1990 Phys. Rev. A 41 426 Google Scholar
[38]	Kodama Y, Romagnoli M, Wabnitz S, Midrio M 1994 Opt. Lett. 19 165 Google Scholar
[39]	Höök A, Karlsson M 1993 Opt. Lett. 18 1388 Google Scholar
[40]	Karpman V I 1996 Phys. Rev. E 53 R1336 Google Scholar
[41]	Roy S, Bhadra S K, Agrawal G P 2009 Opt. Commun. 282 3798 Google Scholar
[42]	Blanco-Redondo A, Eades D, Li J, Lefrancois S, Krauss T F, Eggleton B J, Husko C 2014 Optica 1 299 Google Scholar
[43]	Blanco-Redondo A, Husko C, Eades D, Zhang Y, Li J, Krauss T F, Eggleton B J 2014 Nat. Commun. 5 3160 Google Scholar
[44]	Hasegawa A, Tappert F 1973 Appl. Phys. Lett. 23 142 Google Scholar
[45]	Lo C W, Stefani A, de Sterke C M, Blanco-Redondo A 2018 Opt. Express 26 7786 Google Scholar
[46]	Tam K K K, Alexander T J, Blanco-Redondo A, de Sterke C M 2019 Opt. Lett. 44 3306 Google Scholar
[47]	Kelly S M J 1992 Electron. Lett. 28 806 Google Scholar
[48]	Runge A F J, Qiang Y L, Alexander T J, Rafat M Z, Hudson D D, Blanco-Redondo A, de Sterke C M 2021 Phys. Rev. Res. 3 013166 Google Scholar
[49]	Widjaja J, Kobakhidze E, Cartwright T R, Lourdesamy J P, Runge A F J, Alexander T J, de Sterke C M 2021 Phys. Rev. A 104 043526 Google Scholar
[50]	Zhang Z X, Luo M, Chen J X, Liu M, Luo A P, Xu W C, Luo Z C 2022 Opt. Lett. 47 1750 Google Scholar
[51]	Soto-Crespo J M, Grapinet M, Grelu P, Akhmediev N 2004 Phys. Rev. E 70 066612 Google Scholar
[52]	Liu K W, Yao S Y, Yang C X 2021 Opt. Lett. 46 993 Google Scholar

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