journal article·2024-03-10Open access

Brief Review of Recent Developments in Fiber Lasers

Galina Nemova

Applied Sciences· Volume 14· Issue 6

Abstract

This review covers the recent achievements in high-power rare earth (RE)-doped fiber lasers, Raman fiber lasers, and Brillouin fiber lasers. RE-doped fiber lasers have many applications such as laser cutting, laser welding, laser cleaning, and laser precision processing. They operate in several wavelength ranges including 1050–1120 nm (ytterbium-doped fiber lasers), 1530–1590 nm (erbium- and erbium–ytterbium-doped fiber lasers), and 1900–2100 nm (thulium- and holmium-doped fiber lasers). White spaces in the wavelength spectrum, where no RE-doped fiber lasers are available, can be covered by Raman lasers. The heat power generated inside the laser active medium due to the quantum defect degrades the performance of the laser causing, for example, transverse-mode instability and thermal lensing. It can even cause catastrophic fiber damage. Different approaches permitting the mitigation of the heat generation process are considered in this review. Brillouin fiber lasers, especially multiwavelength Brillouin fiber lasers, have several important applications including optical communication, microwave generation, and temperature sensing. Recent progress in Brillouin fiber lasers is considered in this review.
Source: crossref · Quality: baseline

Research context

OpenAlex topics: Optical properties and cooling technologies in crystalline materials · Spectroscopy and Laser Applications · Solid State Laser Technologies

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Department of Engineering Physics, Polytechnique Montréal, P.O. Box 6079, Station Centre-Ville, Montreal, QC H3C 3A7, Canada

References (100+)

Show source-provided references
1. Kepler, J. (1611). Dioptrice.
2. Huygens, C. (1690). Traité de la Lumière, Gressner & Schramm.
3. An improved method of and means for producing optical images
4. A new method of transporting optical images without aberrations10.1038/173039a0 ↗
5. Demonstration of a new gastroscope, the fiberscope10.1016/S0016-5085(19)35579-9 ↗
6. Fiber Optics. VI. Image Quality and Optical Insulation10.1364/JOSA.49.000779 ↗
7. Dielectric-fibre surface waveguides for optical frequencies10.1049/piee.1966.0189 ↗
8. Ultimate low-loss single-mode fibre at l.55 μm10.1049/el:19790077 ↗
9. Raman oscillation in glass optical waveguide10.1063/1.1654046 ↗
10. Stimulated Brillouin scattering in optical fibers10.1063/1.1654249 ↗
11. Optical power handling capacity of low loss optical fibers as determined by stimulated Raman and Brillouin scattering10.1364/AO.11.002489 ↗
12. Transmission of Stationary Nonlinear Optical Pulses in Dispersive Dielectric Fibers. I. Anomalous Dispersion10.1063/1.1654836 ↗
13. Optical maser action of Nd3+ in a barium crown glass10.1103/PhysRevLett.7.444 ↗
14. Desurvire, E. (1994). Erbium-Doped Fiber Amplifiers: Principles and Applications, John Wiley & Sons, Inc.
15. Theory of Bragg fiber10.1364/JOSA.68.001196 ↗
16. All-silica single-mode optical fiber with photonic crystal cladding10.1364/OL.21.001547 ↗
17. Theoretical analysis of the heat dissipation mechanism in Yb3+-doped double-clad fiber lasers10.1080/09500340701477784 ↗
18. Nemova, G., and Kashyap, R. (2010, January 23–28). High-power fiber lasers with integrated rare-earth optical cooler. Proceedings of the SPIE Laser Refrigeration of Solids III, San Francisco, CA, USA.10.1117/12.840752 ↗
19. Theoretical analysis of heat distribution in Raman fiber lasers and amplifiers employing pure passive fiber10.1109/JPHOT.2020.3038350 ↗
20. Highly nonlinear near-resonant photodarkening in a thulium-doped aluminosilicate glass fiber10.1364/OL.18.000799 ↗
21. Photodarkening in Tb3+-doped phosphosilicate and germanosilicate optical fibers10.1364/OL.19.000874 ↗
22. Science and technology of laser glass10.1016/0022-3093(90)90786-L ↗
23. Multiphonon relaxation of rare-earth ions in oxide glasses10.1103/PhysRevB.16.10 ↗
24. Multiphonon relaxation rates and fluorescence lifetimes for Tm3+ in four oxide glasses10.1016/0009-2614(77)80580-0 ↗
25. Gschneidner, K.A., and Eyring, L. (1987). Handbook on the Physics and Chemistry of Rare Earths, Elsevier.
26. Nemova, G. (2022). Field Guide to Light-Matter Interaction, SPIE Press.10.1117/3.2611513.ch15 ↗
27. Nemova, G. (2019). Field Guide to Laser Cooling Methods, SPIE Press.10.1117/3.2538938.ch3 ↗
28. Laser without internal heat generation10.1109/3.737628 ↗
29. Zwei Bemerkungen über den Unterschied von Lumineszenz- und Temperaturstrahlung10.1007/BF01340652 ↗
30. Athermal continuous-wave fiber amplifier10.1016/j.optcom.2009.03.038 ↗
31. Fiber amplifier with integrated optical cooler10.1364/JOSAB.26.002237 ↗
32. Raman fiber amplifier with integrated cooler10.1109/JLT.2009.2033390 ↗
33. FDTD modeling of excitation-balanced, mJ-level pulse amplifiers in Yb-doped double-clad optical fibers10.1364/OE.495042 ↗
34. A radiation-balanced silica fiber amplifier10.1103/PhysRevLett.127.013903 ↗
35. Laser cooling of solids10.1088/0034-4885/73/8/086501 ↗
36. Nemova, G. (2021). Radiation-Balanced Lasers: History, Status, Potential. Appl. Sci., 11.10.3390/app11167539 ↗
37. 1-kilowatt CW all-fiber laser oscillator pumped with wavelength-beam-combined diode stacks10.1364/OE.20.003296 ↗
38. 1.5 kW, near diffraction-limited, high-efficiency, single-end-pumped all-fiber-integrated laser oscillator10.1364/AO.53.008055 ↗
39. 2 kW single-mode fiber laser with 20-m long delivery fiber and high SRS suppression
40. 1.63 kW monolithic continuous-wave single-mode fiber laser oscillator
41. Mitigating transverse mode instability in all fiber laser oscillator and scaling power up to 2.5 kW employing bidirectional-pump scheme10.1364/OE.24.027828 ↗
42. 3 kW single stage all-fiber Yb-doped single-mode fiber laser for highly reflective and highly thermal conductive materials processing
43. 5-kW single stage all-fber Yb-doped single-mode fiber laser for materials processing
44. 3.05 kW monolithic fiber laser oscillator with simultaneous optimizations of stimulated Raman scattering and transverse mode instability10.1088/2040-8986/aa9ec0 ↗
45. 4.05 kW monolithic fiber laser oscillator based on home-made large mode area fiber Bragg gratings10.3788/COL201816.031407 ↗
46. Extremely robust femtosecond written fiber Bragg gratings for an ytterbium-doped fiber oscillator with 5 kW output power10.1364/OL.389427 ↗
47. 8-kW single-stage all-fiber Yb-doped fiber laser with a BPP of 0.50 mm-mrad
48. The output power of the all-fiber laser oscillator exceeds 7 kW
49. High-efficient kW-level single-mode ytterbium fiber lasers in all-fiber format with diffraction-limited beam at wavelengths in 1000–1030 nm spectral range
50. 75 W 40% efficiency single-mode all-fiber erbium-doped laser cladding pumped at 976 nm10.1364/OL.38.002230 ↗
51. 264 W output power at 1585 nm in Er-Yb co-doped fiber laser using in-band pumping10.1364/OL.39.003974 ↗
52. Yb-free Er-doped all-fiber amplifier cladding-pumped at 976 nm with output power in excess of 100 W
53. Single frequency 1560 nm Er:Yb fiber amplifier with 207 W output power and 50.5% slope efficiency
54. Single-frequency fiber amplifier at 1.5 μm with 100 W in the linearly-polarized TEM00 mode for next-generation gravitational wave detectors10.1364/OE.25.024880 ↗
55. Highly efficient Er–Yb co-doped double-clad fiber amplifier with an Yb-band resonant cavity10.1088/1612-202X/aa568f ↗
56. 656 W Er-doped, Yb-free large-core fiber laser10.1364/OL.43.003080 ↗
57. 302 W single-mode power from an Er/Yb fber MOPA10.1364/OL.392786 ↗
58. 100-W-level single-mode ytterbium-free erbium fiber laser10.1364/OL.427291 ↗
59. 219.6 W large-mode-area Er: Yb co-doped fiber amplifier operating at 1600 nm pumped by 1018 nm fiber lasers10.1364/OL.424368 ↗
60. Highpower and high-brightness Er: Yb co-doped fiber MOPA operating at 1535 nm10.1364/OE.458211 ↗
61. Er/Yb co-doped 345-W all-fiber laser at 1535 nm using hybrid fiber
62. 152 W average power Tm-doped fiber CPA system10.1364/OL.39.004671 ↗
63. Monolithic thulium fiber laser with 567 W output power at 1970 nm10.1364/OL.41.002632 ↗
64. 300 W-level, wavelength-widely-tunable, all-fber integrated thulium-doped fiber laser10.1364/OE.24.011085 ↗
65. 342 W narrow-linewidth continuous-wave thulium-doped all-fber laser10.7498/aps.65.194209 ↗
66. Ultrafast thulium fber laser system emitting more than 1 kW of average power10.1364/OL.43.005853 ↗
67. 790 W incoherent beam combination of a Tm-doped fiber laser at 1941 nm using a 3 × 1 signal combiner10.1364/AO.57.005574 ↗
68. 406 W narrow-linewidth all-fiber amplifier with Tm-doped fiber fabricated by MCVD10.1109/LPT.2019.2946630 ↗
69. 530 W all-fiber continuous-wave Tm-doped fiber laser10.7498/aps.69.20200466 ↗
70. Diffraction limited 195-W continuous wave laser emission at 2.09 μm from a Tm3+, Ho3+ co-doped single-oscillator monolithic fiber laser10.1364/OE.416443 ↗
71. Widely-tunable all-fiber Tm doped MOPA with > 1 kW of output power10.1364/OE.494015 ↗
72. High power resonantly pumped holmium-doped fiber sources
73. IPG Photonics (2024, February 08). “High Power CW Fiber Lasers”. (IPG Photonics). Available online: https://www.ipgphotonics.com/en/products/lasers/highpower-cw-fiber-lasers.
74. Coherently driven molecular vibrations and light modulation10.1103/PhysRevLett.11.160 ↗
75. Mitigating heat dissipation in Raman lasers using coherent anti-Stokes Raman scattering10.1103/PhysRevLett.99.093903 ↗
76. Mitigating heat dissipation in near- and mid-infrared silicon-based Raman lasers using CARS: I. Theoretical analysis10.1109/JSTQE.2007.896623 ↗
77. Mitigating heat dissipation in near- and mid-infrared silicon-based Raman lasers using CARS: II. Numerical demonstration10.1109/JSTQE.2007.896624 ↗
78. Raman-resonant four-wave mixing and energy transfer10.1364/JOSAB.7.000234 ↗
79. Heat Evacuation from Active Raman Media Using Frequency-Selective Dissipative Coupling10.1103/PhysRevResearch.3.013050 ↗
80. Highpower and widely tunable all-fiber Raman laser10.1109/JLT.2008.922337 ↗
81. Ultralow-quantum-defect Raman laser based on the boson peak in phosphosilicate fiber10.1364/PRJ.390950 ↗
82. More than 200 W random Raman fiber laser with ultra-short cavity length based on phosphosilicate fiber10.1364/OL.44.001801 ↗
83. Universal link between the boson peak and transverse phonons in glass10.1038/nmat2293 ↗
84. Highly efficient all-fiber continuous-wave Raman graded-index fiber laser pumped by a fiber laser10.1364/OL.43.001027 ↗
85. 1.2 kW clad pumped Raman all-passive-fiber laser with brightness enhancement10.1364/OL.43.004755 ↗
86. Pure passive fiber enabled highly efficient Raman fiber amplifier with record kilowatt power10.1109/ACCESS.2019.2899452 ↗
87. Diffusion de la lumière et des Rayons X par un corps transparent homogène10.1051/anphys/192209170088 ↗
88. Light scattering by inhomogeneous media
89. Stimulated Brillouin scattering and coherent generation of intense hypersonic waves10.1103/PhysRevLett.12.592 ↗
90. CW Brillouin laser10.1063/1.88583 ↗
91. Millimeter wave carrier generation based on a double-Brillouin-frequency spaced fiber laser10.1364/OE.20.013402 ↗
92. L-band multi-wavelength brillouin-raman fber laser with 20-GHz channel spacing10.1080/01468030.2013.878417 ↗
93. Influence of bidirectional cavity structure on the Brillouin Stokes signal characteristics in ring BFL10.1016/j.ijleo.2019.03.096 ↗
94. Generation of efficient 33 GHz optical combs using cascaded stimulated Brillouin scattering effects in optical fiber10.1088/1555-6611/aa6f7f ↗
95. Widely tunable multiwavelength Brillouin-erbium fiber laser with triple Brillouin-shift wavelength spacing10.1016/j.yofte.2017.12.012 ↗
96. Erbium gain effects on Stokes signal performance in a Fabry-Perot Brillouin Erbium fiber laser10.1007/s11082-019-1912-y ↗
97. Widely triple Brillouin frequency shift multiwavelength Brillouin erbium fiber laser
98. Tunable 50 GHz laser comb generation of multiwavelength Brillouin erbium fber laser10.1016/j.optcom.2020.125542 ↗
99. Multiwavelength fiber laser sources with 60 GHz Brillouin frequency shift10.1007/s11082-023-04731-x ↗
100. Wideband multiwavelength Brillouin fiber laser with switchable channel spacing10.1364/AO.484122 ↗