Tungsten disulfide saturable absorber for passively Q-Switched YVO4/Nd:YVO4/YVO4 laser at 1342.2 nm
Source abstract
Abstract
Abstract By using both tungsten disulfide saturable absorber (WS2-SA) and YVO4/Nd:YVO4(0.3 at.%)/YVO4 crystal, a passively Q-switched laser centered at 1342.2 nm is first reported. Stable Q-switched pulses can be obtained. At the pump power of 12 W, a shortest pulse width of 550 ns and a pulse repetition rate of 97 kHz can be observed by a digital oscilloscope, corresponding to maximum pulse energy of 5.55 μJ and pulse peak power of 10.1 W. The results promote the promising applications of WS2-SA in all-solid-state laser at 1.3 μm.
Source: openaire · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: Advanced Fiber Laser Technologies · Solid State Laser Technologies · Laser-Matter Interactions and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (38)
Show source-provided references
1. V:YAG-a new passive Q-switch for diode-pumped solid-state lasers10.1007/s003400050544 ↗
2. Saturable absorber Co2+:MgAl2O4 crystal for Q switching of 1.34-microm Nd3+:YAlO3 and 1.54-microm Er3+: glass lasers10.1364/AO.38.006343 ↗
3. Passive Q-switching of 1.44μm and 1.34μm diode-pumped Nd:YAG lasers with a V:YAG saturable absorber10.1007/s00340-002-1037-y ↗
4. Enhancement of passively Q-switched performance at 1.34 μm with a class of Nd:GdxY1-xVO4 crystals10.1364/OE.18.021551 ↗
5. Pulsed laser output of LD-end-pumped 1.34 μm Nd:GdVO4 laser with Co: LaMgAl11O19 crystal as saturable absorber10.1364/OPEX.13.003883 ↗
6. Co2+:LMA crystal as saturable absorber for a diode-pumped passively Q-switched Nd:YVO4 laser at 1342 nm10.1007/s00340-007-2790-8 ↗
7. Dissipative soliton operation of an ytterbium-doped fiber laser mode locked with atomic multilayer graphene10.1364/OL.35.003622 ↗
8. Stable nanosecond pulse generation from a graphene- based passively Q-switched Yb-doped fiber laser10.1364/OL.36.004008 ↗
9. Amplification of noise-like pulses generated from a graphene-based Tm-doped all-fiber laser10.1364/OE.24.020359 ↗
10. Graphene saturable absorber mirror for ultra-fast-pulse solid-state laser10.1364/OL.36.001948 ↗
11. Graphene oxide absorber for 2 μm passive mode-locking Tm:YAlO3 laser10.1002/lapl.201110087 ↗
12. High repetition rate QML YVO4/Nd:YVO4/YVO4 laser with a reflective MoS2-SA10.1109/LPT.2018.2804349 ↗
13. Broadband few-layer MoS2 saturable absorbers10.1002/adma.201306322 ↗
14. Ultrafast saturable absorption of two-dimensional MoS2 nanosheets10.1021/nn403886t ↗
15. Molybdenum disulfide (MoS2) as a broadband saturable absorber for ultra-fast photonics10.1364/OE.22.007249 ↗
16. Passively Q-switched Nd:YAlO3 nanosecond laser using MoS2 as saturable absorber10.1364/OE.22.028934 ↗
17. 1-, 1.5-, and 2-μm fiber lasers Q-switched by a broadband few-layer MoS2 saturable absorber10.1109/JLT.2014.2362147 ↗
18. Passively Q-switched and mode-locked YVO4/Nd:YVO4/Nd:YVO4 laser based on a MoS2 saturable absorber at 1342.5 nm10.1016/j.optlastec.2018.08.024 ↗
19. Bi2Se3 Q-switched Nd:YAG ceramic waveguide laser10.1364/OL.40.000637 ↗
20. Ultra-short pulse generation by a topological insulator based saturable absorber10.1063/1.4767919 ↗
21. Topological insulator simultaneously Q-switched dual-wavelength Nd:Lu2O3 laser
22. Mode-locked erbium-doped fiber laser based on evanescent field interaction with Sb2Te3 topological insulator10.1063/1.4885371 ↗
23. Solvothermal synthesis and ultrafast photonics of black phosphorus quantum dots10.1002/adom.201600214 ↗
24. Several nanosecond Nd:YVO4 lasers Q-switched by two dimensional materials: tungsten disulfide, molybdenum disulfide, and black phosphorous10.1364/OE.25.006244 ↗
25. WS2 mode-locked ultrafast fiber laser10.1038/srep07965 ↗
26. WS2 as a saturable absorber for ultrafast photonic applications of mode-locked and Q-switched lasers10.1364/OE.23.011453 ↗
27. Passive Q-switching of a diode-pumped Pr:LiYF4 visible laser using WS2 as saturable absorber10.1109/JPHOT.2016.2550804 ↗
28. Passively q-switched Nd:YAG laser via a WS2 saturable absorber10.1016/j.optcom.2016.01.066 ↗
29. 1.36 W passively Q-switched YVO4/Nd:YVO4 laser with a WS2 saturable absorber10.1109/LPT.2017.2657325 ↗
30. Passively Q-switched Er:LuAG laser at 1.65 μm using MoS2 and WS2 saturable absorbers10.1109/JPHOT.2017.2691740 ↗
31. A 2 micron passively q-switched bulk state pulsed laser based on WS210.1039/C7RA07627D ↗
32. Passively Q-switched Ho,Pr:LiLuF4 bulk laser at 2.95 μm using WS2 saturable absorbers10.1364/OME.7.002090 ↗
33. Self-Q-switched and wavelength-tunable tungsten disulfide-based passively Q-switched Er:Y2O3 ceramic lasers10.1364/PRJ.6.000830 ↗
34. Ana laura elıas, chen-ing chia, bei wang, vincent H. Crespi, florentino lopez-urıas, jean-christophe charlier, humberto terrones, and mauricio terrones, “identification of individual and few layers of WS2 using Raman spectroscopy10.1038/srep01755 ↗
35. Nanosecond pulse generation in a passively Q-switched Nd:GGG laser at 1331 nm by CVD graphene saturable absorber10.1088/2040-8978/17/10/105501 ↗
36. Topological insulator Bi2Se3 based Q-switched Nd:LiYF4 nanosecond laser at 1313 nm10.1364/OE.23.007674 ↗
37. Single- and multi-wavelength Nd:YAlO3 lasers at 1328, 1339 and 1364 nm10.1016/j.optlastec.2016.01.013 ↗
38. High-pulse-energy topological insulator Bi2Te3-based passive Q-switched solid-state laser10.1109/JPHOT.2016.2581490 ↗