基于飞秒激光刻写光纤光栅的研究进展 下载: 2665次
Development of Fiber Gratings Inscribed by Femtosecond Laser
1 国防科技大学前沿交叉学科学院, 湖南 长沙 410073
2 脉冲功率激光技术国家重点实验室, 湖南 长沙 410073
3 高能激光技术湖南省重点实验室, 湖南 长沙 410073
图 & 表
图 1. 逐点刻写的包层模耦合情况[18]
Fig. 1. Transmission spectrum of a point-by-point inscribed FBG[18]
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图 2. 采用逐点刻写的方法制备FBG。 (a)实验装置;(b)刻写在不同位置的不同周期光栅的显微图与光谱;(c)刻写在不同位置相同周期光栅的光谱[21]
Fig. 2. FBG preparation by point-by-point writing. (a)Experimental device; (b) microscope images and reflection spectra of FBGs with different periods written in different positions; (c) spectrum of FBGs with the same period written in different positions[21]
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图 3. 在扭转的七芯光纤上刻写FBG阵列[23]
Fig. 3. FBG array inscription in twist seven-core fiber[23]
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图 4. 采用逐线刻写的方法制备FBG。 (a)飞秒激光逐线刻写示意图;(b)四阶FBG显微示意图;(c)逐线刻写FBG透射谱[24]
Fig. 4. FBG preparation by line-by-line writing. (a) Schematic of femtosecond laser line-by-line inscription; (b) microscopic of fourth-order FBG; (c) transmission spectrum of line-by-line inscribed FBG[24]
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图 5. π相移光栅。(a)光栅在不同偏振态下的透射谱;(b)不同扭转角下,P1-P2的变化曲线[26]
Fig. 5. π phase shift grating. (a) Transmission spectrum of different polarization states; (b) curves of P1-P2 with different twist angles[26]
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图 6. 逐线刻写光栅阵列。(a) FBG阵列编码的3位二进制编码的示意图;(b)编码111的FBG阵列的后向散射[28]
Fig. 6. Line-by-line writing grating array. (a) Schematic diagram of the encoded FBG array with a 3-bit binary coding; (b) backscattering of FBG array with code 111[28]
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图 7. 逐面刻写光栅阵列。(a) FBG阵列[29];(b)倾斜角为7°的TFBG光谱[30]
Fig. 7. Plane-by-plane writing grating array. (a) FBGs array[29]; (b) TFBG spectrum with a tilt angle of 7°[30]
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图 8. 铒镱共掺的双包层光纤上刻写光栅对。(a)光栅光谱图;(b)振荡器光路;(c)斜率效率[33]
Fig. 8. Grating pair on double-clad fiber co-doped with Er and Yb. (a) Spectrum of FBGs; (b) schematic of oscillator; (c) slope efficiency[33]
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图 9. 实验结果。(a) 45°倾斜光栅插损与偏振相关损耗;(b)非线性偏振旋转锁模光路;(c)单孤子锁模光谱;(d)单孤子锁模自相关;(e)类噪声锁模光谱;(f)类噪声锁模自相关[34]
Fig. 9. Experimental results. (a) Polarization dependent loss and insertion loss of 45° tilt grating; (b) schematic of NPR mode-locked fiber laser; (c) optical spectrum of single-soliton mode-locked fiber laser; (d) autocorrelation of single-soliton mode-locked fiber laser; (e) optical spectrum of noise-like mode-locked fiber laser; (f) autocorrelation of noise-like mode-locked fiber laser[34]
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图 10. 实验结果。(a)逐面刻写光栅的光路;(b) type I型FBG光谱;(c)改变重复频率实现type I型CFBG刻写; (d) type II型FBG光谱[35]
Fig. 10. Experimental results. (a) Schematic of plane-by-plane inscription; (b) spectrum of type I FBG; (c) spectrum of type I CFBG; (d) spectrum of type II FBG[35]
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图 11. 纤芯扫描技术。(a)示意图;(c)纤芯扫描与逐点刻写的FBG光谱对比[36]
Fig. 11. Core-scanning technology. (a) Schematic of core-scanning; (b) FBG spectrum comparison of core-scanning and point-by-point [36]
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图 12. 不同方法刻写的CFBG。(a)逐点刻写;(b)纤芯扫描;(c)改进型纤芯扫描;(d)逐点刻写CFBG的光谱;(e)纤芯扫描刻写CFBG的光谱;(f)改进纤芯扫描刻写CFBG的光谱[37]
Fig. 12. CFBG written by different methods. (a) Point-by-point; (b) core-scanning; (c) modified core-scanning spectrum of CFBG by point-by-point; (d) spectrum of CFBG by core-scanning; (e) spectrum of CFBG by modified core-scanning[37]
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图 13. 双芯少模光栅。(a)实验光路;(b)局部放大图[41]
Fig. 13. Twin-core FMFBG. (a) Experimental optical path; (b) partial enlarged view[41]
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图 14. TMFBG。(a)刻写TMFBG示意图;(b)TMFBG光谱图[45]
Fig. 14. TMFBG. (a) Schematic of TMFBG inscription; (b) spectrum of TMFBG[45]
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图 15. 实验结果。(a)保留涂敷层(蓝)与去除涂敷层(黑)的光谱;(b)斜率效率与实验光路[47]
Fig. 15. Experimental results. (a) Spectrum of FBG (blue is with coating, black is without coating);(b) slope efficiency and schematic of oscillator[47]
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图 16. 在未去涂敷层的光纤上刻写FBG。(a)刻写光栅光路;(b)重复频率为1 kHz,曝光时间为5 min的光谱;(c)重复频率为500 Hz,曝光时间为10 min的光谱[49]
Fig. 16. Writing FBG on the optical fiber without decoating. (a) Schematic of FBG inscription; (b) spectrum of FBG with repetition rate 1 kHz and exposure time 5 min; (c) spectrum of FBG with repetition rate 500 Hz and exposure time 10 min[49]
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图 17. 飞秒激光相位模板扫描技术。(a)相位模板扫描刻写示意图;(b)光栅透射谱以及透射深度随光栅长度的变化[50]
Fig. 17. Femtosecond laser phase template scanning technology. (a) Schematic of phase mask scanning technology; (b) transmission spectra and transmission over length[50]
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图 18. 相位模板扫描技术。(a)掺铒光纤刻写FBG透射谱;(b)激光器示意图;(c)斜率效率[51]
Fig. 18. Phase mask scanning technology. (a) Transmission spectrum of FBG in EDF; (b) laser experiment setup; (c) slope efficiency[51]
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图 19. 实验结果。(a) CFBG光谱;(b)激光器光路;(c)高功率激光器斜率效率[53]
Fig. 19. Experimental results. (a) Spectrum of CFBG; (b) laser experiment setup; (c) slope efficiency[53]
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图 20. 实验结果。(a)内包层CFBG光谱;(b)激光器光路[54]
Fig. 20. Experimental results. (a) Spectrum of inner-cladding CFBG; (b) laser experiment setup[54]
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表 1不同飞秒激光直写方式的对比
Table1. Comparison of various femtosecond laser direct inscribing methods
Method | Point-by-point | Line-by-line | Plane-by-plane | Core-scanning |
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Alignment | Extremely high | High | Low | High | Pulse energy /(nJ/pulse) | 50—500 | 100 | 100 | 100 | Insertion loss | High IL at shorterwavelength | High IL at shorterwavelength | Low IL | Low IL | Application | Sensors(especially hightemperature sensors) | Sensing by birefringencecharacteristics | Sensors andlasers | Sensors |
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表 2相位模板刻写技术的对比
Table2. Comparison between phase mask writing methods
Method | Static inscription | Dynamic inscription |
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Stability requirements | Low | High | System complexity | Low | High | Inscription time | Short | Long | Grating length | Limited by beam diameter | Limited by phase mask | Application | Sensors | High power fiber laser |
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表 3国内外飞秒激光刻写光纤光栅的进展情况
Table3. Development of fiber gratings inscribed by using femtosecond laser
Reference | λfs /nm | f /kHz | T /fs | E /nJ | Description | P /μm | λR /nm |
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[15] | 800 | 200 | 120 | | First reported PBPLPG | DW | 1100-1700 | [16] | 800 | 1 | 150 | 300-1000 | First reported PBP FBG | DW | 1550 | [17] | 800 | 1 | 120 | 160-300 | Loss mechanism of PBP | DW | 1550 | [18] | 800 | | 110 | 200-275 | Cladding mode coupling | DW | 1540 | [19] | 800 | | | 80-350 | Impact of scattering loss on FBG reflectivity | DW | 1550 | [20] | 800 | 1 | 100 | 200 | Sampling FBG with hightemperature resistance | DW | 1550 | [21] | 800 | 1 | 100 | 200 | Parallel-integrated FBGs | DW | 1550 | [22] | 800 | 1 | 100 | 59-174 | Mie scattering suppression in PBP FBG | DW | 1550 | [23] | 1030 | 1 | 232 | 200 | Bending sensing by seven cores FBG | DW | 1550 | [24] | 800 | 1 | 110 | 85 | LBL inscribed low IL and PDL FBG | DW | 1600 | [25] | 266 | 1 | 120 | 4×106(maxima) | High birefringence FBGby LBL inscription | DW | 1550 | | 520 | 200 | 400 | | LBL polarization-dependentπ-PSFBG for twist sensing | DW | 1550 | [27] | | | | 130 | π-PSFBG for strain sensing | DW | 1550 | [28] | 513 | 200 | 250 | 14 | LBL inscribed fiber label | DW | 1550 | [29] | | 4 | | 100 | FBGs array for vibration sensor | DW | 1550 | [30] | 517 | 50 | 220 | 100 | High order resonance of TFBG | DW | 1560 | [31] | 517 | 5 | 220 | 80 | Polymer fiber grating sensor | DW | 1550 | [32] | 517 | | 220 | | Polymer fiber grating sensor | DW | 1550 | [33] | 517 | 100 | 220 | 150 | FBGs in oscillator | DW | 1560 | [34] | 517 | 50 | 217 | 150 | NPR mode locked by 45° TFBG | DW | 1560 | [35] | 800 | 0.25 | 120 | 1400-1900 | Beam expanding Pl-B-Pl | DW | 1550 | [36] | 800 | 1 | 120 | 117 | Core-scanning Low loss FBG | DW | 1540 | [37] | 800 | 0.1-1 | 112 | 83-200 | Core-scanning CFBG | DW | 1540 | [38] | 800 | 0.01、1 | 120 | 3×105 | First report of femtosecond laser andphase mask inscribed FBG | 4.284, 3.213,2.142, 1.071 | 1550 | [39] | 800 | 0.125 | 125 | 6×105 | Cladding mode suppression byfocal point scanning | 3.213 | 1550 | [40] | 800 | 1 | 100 | 1.08×105-2.67×105 | Negative refractiveindex FBG | 1.070 | 1550 | [41] | 800 | 1 | 100 | 1.02×105 | Double cores FBG | 1.070 | 1550 | [42] | 800 | 1 | 100 | 2×105 | PCFBG for refractiveindex sensing | 1.070 | 1550 | [43] | 800 | 0.1 | | 0.4×106-0.5×106 | Higher order resonance | 1.071 | 600-1700 | [44] | 800 | 1 | 50 | 4.2×105 | Cladding mode resonancein two mode fiber | 2.142 | 1550 | [45] | 800 | 1 | 35 | 4×106(maxima) | Cladding mode resonancein two mode fiber | 2.142 | 1550 | [46] | 1030 | 0.1 | 190 | | PCFBG | 2.175 | 1560 | [47] | 266 | 1 | 40 | | Oscillator used FBG inscriptionwithout coating removing | 1.0742 | 1550 | [48] | 800 | 1 | 80 | 0.78×106;1.1×106 | Strong cladding mode resonantFBG by beam expanding | 1.07 | 1300-1550 | [49] | 800 | 0.2-1 | 35 | 0.4×106 | focal point scanning FBGwithout coating removing | 2.14 | 1550 | [50] | 800 | 1 | 50 | 2×105,6×105 | phase mask scanning FBG | 2.15 | 1555 | [51] | 800 | 1 | 50 | 6×105 | High reflection FBG onEDF for oscillator | 2.15 | 1555 | [52] | 800 | | 120 | | Oscillator with514 W output | | 1078.7 | [53] | 800 | | 100 | | Oscillator with1.9 kW output | | 1070 | [54] | 403 | 1 | 30 | 6×106 | Pump reflector | 0.674 | 976 |
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表 4飞秒激光直写与相位模板辅助刻写技术的对比
Table4. Comparison between direct inscribing and phase mask assisted writing
Method | Direct writing | Phase mask assisted writing |
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Pulse energy /(nJ/pulse) | 100 | 0.5 | Resonance wavelength | Arbitrary | Limited by phase mask | IL | High | Low | Flexibility | High | Low | Alignment | High | Low | Repeatability | Low | High | Characteristics of gratings | 1. High polarization-related properties and high birefringence properties2. Easily fabrication of novel gratings by adjusting inscription condition | Stable spectral properties | Application | Novel sensors and quasi-distributed sensors | Sensors and lasers | Developing trend | 1. Inscription of FBGs array with different resonance wavelengths to realize quasi-distributed sensors2. Inscription fiber gratings with special refractive index profile to control mode coupling | Inscription of fiber gratingsin high power oscillator |
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李宏业, 饶斌裕, 赵晓帆, 胡琪浩, 王蒙, 王泽锋. 基于飞秒激光刻写光纤光栅的研究进展[J]. 激光与光电子学进展, 2020, 57(11): 111420. Hongye Li, Binyu Rao, Xiaofan Zhao, Qihao Hu, Meng Wang, Zefeng Wang. Development of Fiber Gratings Inscribed by Femtosecond Laser[J]. Laser & Optoelectronics Progress, 2020, 57(11): 111420.