Effect of Saturable Absorber Length on Characteristics of Dual Laser Pulses of Passive Q-Switched
DOI:
https://doi.org/10.32792/utq/utjsci/v11i1.1151Keywords:
Laser, high Power Pulses, Passive Q-switching, solid-state laserAbstract
The effect of saturable absorber material length on the characteristics of the dual passive Q-switching pulses generated from two wavelengths ( and ) instead of single wavelength was simulated. Numerical solution of our previous rate equations model using Rung-Kutta-Fahelberg method has been utilized in simulation. Nd+3 :YAG using as an active medium, and Cr+4:YAG as a saturable absorber material. The results showed that the Nd+3:YAG dual passive Q-switching generated or released at an advanced(earlier) time and characterized by short duration times, high energy and high power with the increasing in the value of . The passive Q-switching for , are released respectively at time 58ns, 60 ns approximately at , while released at time 34 ns, 36 ns respectively approximately at . The duration time of , pulses approximate to 16.8ns, 14.6 ns respectively at , while approximate to 10.8 ns ,9.2 ns respectively at .
Received: 2023-12-17
Revised: 2024-01-21
Accepted: 2024-01-24
References
. Y. Shen, X. Fu, C.Yao ,W. Li , Y.Wang, X.Zhao , Y.Ning. “ Optical Crystals for 1.3 μm All-Solid-State Passively Q-Switched Laser”. Crystals. 29;12(8):1060. Jul 2022.
X.Zhang , K.Zhong , H.Qiao, Y. Zheng, F.Li, D.Xu, J.Yao. “A passively Q-switched dual-wavelength laser with pulsed LD coaxial end-pumped configuration”. InAdvanced Lasers, High-Power Lasers, and Applications XIII (Vol. 12310, pp. 24-30). SPIE. Dec 28, 2022.
. Z.Ali , Z.Abdulsada , N.Arasavalli, S.Kadhim, & H. Akram “Initial Transmission Influence on Saturable Absorber Absorption Activity of Passive Q-Switching Erbium-Doped Fiber Laser System”. University of Thi-Qar Journal of Science, 10(2), 224-229. (2023).
. M.Li , Y.Qin, C.Wang , X.Liu , S.Long, X.Tang , T.Wen. “Nonuniform pumped passively Q-switched laser using Nd: YAG/Cr+4: YAG composite crystal with high-pulse energy”. Optical Engineering. 1;58(3):036106-. Mar 2019.
. H.Tanaka , C.Kränkel, F.Kannari . “Transition-metal-doped saturable absorbers for passive Q-switching of visible lasers”. Optical Materials Express. 1;10(8):1827-42. Aug 2020.
. W.Koechner. Solid-state laser engineering. Springer; Nov 11, 2013.
R.Yan , Y.Zhou, X.Li, Y.Liu, Y.Jiang, W.Yao, F.Peng, Q.Zhang, R.Dou, J.Gao. “4F3/2→ 4I9/2 and 4F3/2→ 4I13/2 laser operations with a Nd: GdTaO4 crystal”. Optics & Laser Technology. 1;131:106444. Nov 2020.
MA. Mahmood, SR.Mahdi. “Numerical Analysis of a Lasing Output for the Quasi _ Three _ Level Thin Disk Lasers”. InJournal of Physics: Conference Series. 2021 May 1 (Vol. 1879, No. 3, p. 032116). IOP Publishing. May 2021.
Chen F, Sun J, Yan R, Yu X. "Reabsorption cross section of Nd3+-doped quasi-three-level lasers". Scientific reports. 4;9(1):5620. Apr 2019.
Ma C, Zhu J, Hu Z, Wen Z, Long J, Yuan X, Cao Y. Spectroscopic Properties and Continuous Wave Laser Performances at 1064 nm of Nd3+: LuAG Transparent Ceramic. IEEE Photonics Journal. 15;9(2):1-4. Mar 2017
A.Sara, M. Abdul kareem."Rate Equations Model to Simulate the Dual Generation of Nd+3: YAG Passive Q-swiched Laser Pulses”, Indian Journal of Science and Technology, 27-10-: 3462-3470. (40)2023. https://doi.org/ 10.17485/IJST/v16i40.1748
S. Bassem Kadhem and A. Mahdi Salih," Simulation of Raman spontaneous scattering factor effect on Stoke Raman and passive Q-switching pulses characteristic”, IOP Conference Series: Materials Science and Engineering, 928,doi:10.1088/1757-899X/928/7/072160. 2020.
K. Semwal, SC .Bhatt. “Study of Nd3+ ion as a dopant in YAG and glass laser”. International Journal of Physics. 1(1):15-21. 2013.
Ö. GÜREL. Master of Science Thesis Stockholm, Sweden 2009.
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