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. Comparison of laser wavebands generated by typical fiber gas laser and fiber laser
[1] Fig. 2. Diagrams of energy level transition. (a) Diagram of energy level transition of C2H2 molecules pumped with P branch absorption lines; (b) diagram of energy level transition of CO2 molecules pumped with R branch absorption lines
Fig. 3. Diagram of fiber gas laser based on population inversion
Fig. 4. 3 μm laser generation from acetylene-filled Kagome HCF pumped by OPO
[2]. (a) Experimental setup; (b) output 3 μm laser spectrum
Fig. 5. Single-pass configuration experiment using acetylene-filled anti-resonant HCF pumped by tunable diode laser
[4]. (a) Diagram of experimental setup; (b) laser pulse energy varying with absorbed pump pulse energy at different pressure
Fig. 6. Ring-cavity configuration experiment using acetylene-filled anti-resonant HCF pumped by diode laser
[6].(a) Diagram of experimental setup; (b) output spectra for different pump wavelengths
Fig. 7. Single-pass configuration experiment of fiber acetylene gas CW laser output
[7]. (a) Diagram of experimental setup; (b) output laser power as a function of absorbed pump power at different pressure
Fig. 8. Experiment for measuring output beam quality of fiber acetylene gas laser
[8]. (a) Experimental setup; (b)
M2 value corresponding to different output pulse energy
Fig. 9. Experiment of OPO pumping CO
2-filled silver plating capillary
[1]. (a) Diagram of experimental setup; (b) output spectrum and energy level transition principle
Fig. 10. Experimental setup and results of CO
2 laser based on anti-resonant HCFs
[13]. (a) Diagram of experimental setup; (b) schematic diagram of energy level transition; (c) output spectrum; (d) output power at 4 μm varying with absorbed pump power
Fig. 11. Experiment of thulium-doped fiber amplifier pumping HBr-filled anti-resonant HCF
[14]. (a) Diagram of experimental setup; (b) output spectrum and energy level transition principle
Fig. 12. Experimental setup and output spectrum of CW light pumped I
2 vapor fiber gas laser
[5]. (a) Experimental setup;(b) output laser spectrum
Fig. 13. Experiments of 3 μm laser radiation from electrically excited He-Xe gas based on anti-resonant HCF
[41]. (a) Diagram of experimental setup and output signals for different fiber lengths; (b) output laser spectrum
Fig. 14. Coupling by inserting tapered solid-core fiber into HCF
[47] Fig. 15. Coupling efficiency of tapered fiber and anti-resonant HCF varying with waist diameter
[48]. (a) Coupling efficiency of tapered fiber HI-1060 and ice-cream anti-resonant HCF at 1064 nm varying with waist diameter. Inset is output near field from HCF; (b) coupling efficiency of tapered SMF-28 and node-less anti-resonant HCF at 1568 nm varying with waist diameter
Gas gainmedium | Pumping band | Lasing band |
---|
λ /μm | Vibrational statetransition | Spectral line intensity /(cm·molecule-1) | λ /μm | Vibrational statetransition | Spectral line intensity /(cm·molecule-1) |
---|
C2H2 | 1.51--1.55 | v0→v1+v3 | 1.34×10-20 | 3.09--3.21 | v1+v3→v1 | - | CO | 1.56--1.65 | v=0→v=3 | 2.17×10-23 | 2.32--2.51 | v=3→v=1 | 3.17×10-25 | CO | 2.29--2.52 | v=0→v=2 | 3.47×10-21 | 4.43--5.26 | v=2→v=1 | 2.70×10-23 | CO2 | 1.99--2.06 | v0→2v1+v3 | 1.32×10-21 | 4.25--4.53 | 2v1+v3→2v1 | 7.55×10-24 | N2O | 1.98--2.02 | v0→3v1+2v2 | 5.00×10-23 | 2.65--2.71 | 3v1+2v2→v1 | 5.97×10-24 | HI | 1.53--1.95 | v=0→v=3 | 3.22×10-22 | 4.45--7.49 | v=3→v=2 | 5.00×10-30 | HBr | 1.94--2.72 | v=0→v=2 | 8.30×10-22 | 3.69--6.59 | v=2→v=1 | 5.63×10-25 |
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Table 1. Common gas media and related parameters in mid-infrared fiber gas laser
Pump source | Pumpwavelength /nm | Gas gainmedium | Laserwavelength /μm | Maximum laserenergy or power | Efficiency /% | Ref. No. |
---|
OPO | 1521 | C2H2 | 3.12, 3.16 | 6 nJ | 1 | [2] | OPA | 1532.8 | C2H2 | 3.11, 3.17 | 550 nJ | 20 | [3] | OPA | 1541.3 | HCN | 3.09, 3.15 | 56 nJ | 0.02 | [3] | OPO | 2002.5 | CO2 | 4.30, 4.37 | 100 μJ | 20 | [3] | OPO | 1521 | C2H2 | 3.12, 3.16 | 600 nJ | 27 | [1] | Diode laser | 1530 | C2H2 | 3.12, 3.16 | 0.8 μJ | 30 | [4] | Nd∶Vanadate | 532 | I2 | 1.31, 1.33 | 8 mW | 4 | [5] | Diode laser | 1530 | C2H2 | 3.08--3.18 | 2.5 mW | 6.7 | [6] | Diode laser | 1530 | C2H2 | 3.12, 3.16 | 1.12 W | 33.2 | [7] | OPA | 1530 | C2H2 | 3.11, 3.17 | 1.41 μJ | 20 | [8] | Diode laser | 1530--1535 | C2H2 | 3.09--3.21 | 0.6 μJ0.77 W (CW) | 1613 | [10] | TDFA | 2000.6 | CO2 | 4.30, 4.39 | 80 mW | 19.3 | [13] | OPO | 1517 | N2O | 4.59, 4.66 | 150 nJ | 9 | [12] | Electrodes | | He∶Xe (5∶1) | 3.11, 3.37, 3.51 | | | [41] |
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Table 2. Research progress of fiber gas lasers based on population inversion