Author Affiliations
1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, Hunan 410073, China2State Key Laboratory of Pulsed Power Laser Technology, Changsha, Hunan 410073, China3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha, Hunan 410073, Chinashow less
Fig. 1. Transmission spectrum of a point-by-point inscribed FBG
[18] 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] Fig. 3. FBG array inscription in twist seven-core fiber
[23] 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] Fig. 5. π phase shift grating. (a) Transmission spectrum of different polarization states; (b) curves of
P1-
P2 with different twist angles
[26] 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] Fig. 7. Plane-by-plane writing grating array. (a) FBGs array
[29]; (b) TFBG spectrum with a tilt angle of 7°
[30] 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] 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] 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] Fig. 11. Core-scanning technology. (a) Schematic of core-scanning; (b) FBG spectrum comparison of core-scanning and point-by-point
[36] 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] Fig. 13. Twin-core FMFBG. (a) Experimental optical path; (b) partial enlarged view
[41] Fig. 14. TMFBG. (a) Schematic of TMFBG inscription; (b) spectrum of TMFBG
[45] Fig. 15. Experimental results. (a) Spectrum of FBG (blue is with coating, black is without coating);(b) slope efficiency and schematic of oscillator
[47] 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] Fig. 17. Femtosecond laser phase template scanning technology. (a) Schematic of phase mask scanning technology; (b) transmission spectra and transmission over length
[50] Fig. 18. Phase mask scanning technology. (a) Transmission spectrum of FBG in EDF; (b) laser experiment setup; (c) slope efficiency
[51] Fig. 19. Experimental results. (a) Spectrum of CFBG; (b) laser experiment setup; (c) slope efficiency
[53] Fig. 20. Experimental results. (a) Spectrum of inner-cladding CFBG; (b) laser experiment setup
[54] 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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Table 1. Comparison of various femtosecond laser direct inscribing 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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Table 2. Comparison between phase mask writing methods
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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Table 3. Development of fiber gratings inscribed by using femtosecond laser
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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Table 4. Comparison between direct inscribing and phase mask assisted writing