• Laser & Optoelectronics Progress
  • Vol. 57, Issue 11, 111420 (2020)
Hongye Li1, Binyu Rao1, Xiaofan Zhao1, Qihao Hu1, Meng Wang1、2、3, and Zefeng Wang1、2、3、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, Hunan 410073, China
  • 2State Key Laboratory of Pulsed Power Laser Technology, Changsha, Hunan 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha, Hunan 410073, China
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    DOI: 10.3788/LOP57.111420 Cite this Article Set citation alerts
    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 Copy Citation Text show less
    Transmission spectrum of a point-by-point inscribed FBG[18]
    Fig. 1. Transmission spectrum of a point-by-point inscribed FBG[18]
    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. 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]
    FBG array inscription in twist seven-core fiber[23]
    Fig. 3. FBG array inscription in twist seven-core fiber[23]
    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. 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]
    π phase shift grating. (a) Transmission spectrum of different polarization states; (b) curves of P1-P2 with different twist angles[26]
    Fig. 5. π phase shift grating. (a) Transmission spectrum of different polarization states; (b) curves of P1-P2 with different twist angles[26]
    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. 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]
    Plane-by-plane writing grating array. (a) FBGs array[29]; (b) TFBG spectrum with a tilt angle of 7°[30]
    Fig. 7. Plane-by-plane writing grating array. (a) FBGs array[29]; (b) TFBG spectrum with a tilt angle of 7°[30]
    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. 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]
    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. 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]
    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. 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]
    Core-scanning technology. (a) Schematic of core-scanning; (b) FBG spectrum comparison of core-scanning and point-by-point [36]
    Fig. 11. Core-scanning technology. (a) Schematic of core-scanning; (b) FBG spectrum comparison of core-scanning and point-by-point [36]
    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. 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]
    Twin-core FMFBG. (a) Experimental optical path; (b) partial enlarged view[41]
    Fig. 13. Twin-core FMFBG. (a) Experimental optical path; (b) partial enlarged view[41]
    TMFBG. (a) Schematic of TMFBG inscription; (b) spectrum of TMFBG[45]
    Fig. 14. TMFBG. (a) Schematic of TMFBG inscription; (b) spectrum of TMFBG[45]
    Experimental results. (a) Spectrum of FBG (blue is with coating, black is without coating);(b) slope efficiency and schematic of oscillator[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]
    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. 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]
    Femtosecond laser phase template scanning technology. (a) Schematic of phase mask scanning technology; (b) transmission spectra and transmission over length[50]
    Fig. 17. Femtosecond laser phase template scanning technology. (a) Schematic of phase mask scanning technology; (b) transmission spectra and transmission over length[50]
    Phase mask scanning technology. (a) Transmission spectrum of FBG in EDF; (b) laser experiment setup; (c) slope efficiency[51]
    Fig. 18. Phase mask scanning technology. (a) Transmission spectrum of FBG in EDF; (b) laser experiment setup; (c) slope efficiency[51]
    Experimental results. (a) Spectrum of CFBG; (b) laser experiment setup; (c) slope efficiency[53]
    Fig. 19. Experimental results. (a) Spectrum of CFBG; (b) laser experiment setup; (c) slope efficiency[53]
    Experimental results. (a) Spectrum of inner-cladding CFBG; (b) laser experiment setup[54]
    Fig. 20. Experimental results. (a) Spectrum of inner-cladding CFBG; (b) laser experiment setup[54]
    MethodPoint-by-pointLine-by-linePlane-by-planeCore-scanning
    AlignmentExtremely highHighLowHigh
    Pulse energy /(nJ/pulse)50—500100100100
    Insertion lossHigh IL at shorterwavelengthHigh IL at shorterwavelengthLow ILLow IL
    ApplicationSensors(especially hightemperature sensors)Sensing by birefringencecharacteristicsSensors andlasersSensors
    Table 1. Comparison of various femtosecond laser direct inscribing methods
    MethodStatic inscriptionDynamic inscription
    Stability requirementsLowHigh
    System complexityLowHigh
    Inscription timeShortLong
    Grating lengthLimited by beam diameterLimited by phase mask
    ApplicationSensorsHigh power fiber laser
    Table 2. Comparison between phase mask writing methods
    Referenceλfs /nmf /kHzT /fsE /nJDescriptionP /μmλR /nm
    [15]800200120First reported PBPLPGDW1100-1700
    [16]8001150300-1000First reported PBP FBGDW1550
    [17]8001120160-300Loss mechanism of PBPDW1550
    [18]800110200-275Cladding mode couplingDW1540
    [19]80080-350Impact of scattering loss on FBG reflectivityDW1550
    [20]8001100200Sampling FBG with hightemperature resistanceDW1550
    [21]8001100200Parallel-integrated FBGsDW1550
    [22]800110059-174Mie scattering suppression in PBP FBGDW1550
    [23]10301232200Bending sensing by seven cores FBGDW1550
    [24]800111085LBL inscribed low IL and PDL FBGDW1600
    [25]26611204×106(maxima)High birefringence FBGby LBL inscriptionDW1550
    520200400LBL polarization-dependentπ-PSFBG for twist sensingDW1550
    [27]130π-PSFBG for strain sensingDW1550
    [28]51320025014LBL inscribed fiber labelDW1550
    [29]4100FBGs array for vibration sensorDW1550
    [30]51750220100High order resonance of TFBGDW1560
    [31]517522080Polymer fiber grating sensorDW1550
    [32]517220Polymer fiber grating sensorDW1550
    [33]517100220150FBGs in oscillatorDW1560
    [34]51750217150NPR mode locked by 45° TFBGDW1560
    [35]8000.251201400-1900Beam expanding Pl-B-PlDW1550
    [36]8001120117Core-scanning Low loss FBGDW1540
    [37]8000.1-111283-200Core-scanning CFBGDW1540
    [38]8000.01、11203×105First report of femtosecond laser andphase mask inscribed FBG4.284, 3.213,2.142, 1.0711550
    [39]8000.1251256×105Cladding mode suppression byfocal point scanning3.2131550
    [40]80011001.08×105-2.67×105Negative refractiveindex FBG1.0701550
    [41]80011001.02×105Double cores FBG1.0701550
    [42]80011002×105PCFBG for refractiveindex sensing1.0701550
    [43]8000.10.4×106-0.5×106Higher order resonance1.071600-1700
    [44]8001504.2×105Cladding mode resonancein two mode fiber2.1421550
    [45]800135106(maxima)Cladding mode resonancein two mode fiber2.1421550
    [46]10300.1190PCFBG2.1751560
    [47]266140Oscillator used FBG inscriptionwithout coating removing1.07421550
    [48]8001800.78×106;1.1×106Strong cladding mode resonantFBG by beam expanding1.071300-1550
    [49]8000.2-1350.4×106focal point scanning FBGwithout coating removing2.141550
    [50]8001502×105,6×105phase mask scanning FBG2.151555
    [51]8001506×105High reflection FBG onEDF for oscillator2.151555
    [52]800120Oscillator with514 W output1078.7
    [53]800100Oscillator with1.9 kW output1070
    [54]4031306×106Pump reflector0.674976
    Table 3. Development of fiber gratings inscribed by using femtosecond laser
    MethodDirect writingPhase mask assisted writing
    Pulse energy /(nJ/pulse)1000.5
    Resonance wavelengthArbitraryLimited by phase mask
    ILHighLow
    FlexibilityHighLow
    AlignmentHighLow
    RepeatabilityLowHigh
    Characteristics of gratings1. High polarization-related properties and high birefringence properties2. Easily fabrication of novel gratings by adjusting inscription conditionStable spectral properties
    ApplicationNovel sensors and quasi-distributed sensorsSensors and lasers
    Developing trend1. Inscription of FBGs array with different resonance wavelengths to realize quasi-distributed sensors2. Inscription fiber gratings with special refractive index profile to control mode couplingInscription of fiber gratingsin high power oscillator
    Table 4. Comparison between direct inscribing and phase mask assisted writing
    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
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