Dark soliton generation using dual Brillouin fiber laser in a fiber optic ring resonator

2010 ◽  
Vol 52 (4) ◽  
pp. 881-883 ◽  
Author(s):  
S. F. Hanim ◽  
J. Ali ◽  
P. P. Yupapin
2015 ◽  
Vol 47 (8) ◽  
pp. 2455-2464 ◽  
Author(s):  
I. S. Amiri ◽  
M. R. K. Soltanian ◽  
S. E. Alavi ◽  
H. Ahmad

2021 ◽  
Vol 11 (1) ◽  
pp. 407
Author(s):  
Jinho Lee ◽  
Ju Han Lee

This study reports a Q-switching-based, 2058-nm holmium (Ho) fiber laser incorporating a saturable absorber (SA) based on graphene oxide (GO). The SA was prepared with a side-polished fiber, while GO particles were deposited onto the fiber-polished surface to realize an all-fiber SA. A continuous-wave thulium-doped all-fiber laser, which was configured with a master-oscillator power-amplifier (MOPA) structure, was constructed as a pumping source. By inserting the fabricated SA into an all-fiber ring resonator based on 1-m length of Ho-doped fiber, Q-switched pulses could readily be obtained at a wavelength of 2058 nm. The pulse width was observed to vary from 2.01 to 1.56 μs as the pump power was adjusted from ~759 to 1072 mW, while the repetition rate was tunable from 45.56 to 56.12 kHz. The maximum values of average optical power and pulse energy were measured as ~11.61 mW and 207.05 nJ, respectively, at a ~1072 mW pump power.


2017 ◽  
Vol 405 ◽  
pp. 253-258 ◽  
Author(s):  
Dmitry A. Korobko ◽  
Igor O. Zolotovskii ◽  
Krassimir Panajotov ◽  
Vasily V. Spirin ◽  
Andrei A. Fotiadi

2014 ◽  
Vol 34 (5) ◽  
pp. 0514002
Author(s):  
程成 Cheng Cheng ◽  
袁芳 Yuan Fang

2020 ◽  
Vol 10 (4) ◽  
pp. 291-297
Author(s):  
Weiren Cheng ◽  
Tianming Luo ◽  
Linghao Cheng ◽  
Hao Liang ◽  
Bai-ou Guan

Abstract A compact fiber-optic magnetic field sensor is proposed by packaging an orthogonal dual-frequency fiber grating laser and a copper wire with alternating electrical current together inside epoxy resin. The alternating current generates Ampere force in a magnetic field, which changes the birefringence of the fiber laser and hence tunes the frequency of the beat signal after photodetection. The magnetic field magnitude can then be detected by measuring the frequency change of the beat signal. The sensitivity of the sensor can be tuned with a maximum response of 35.21 kHz/kGs demonstrated. Moreover, the sensor shows good immunity to environment interference.


2020 ◽  
Vol 126 ◽  
pp. 106068
Author(s):  
L.A. Rodríguez-Morales ◽  
B. Ibarra-Escamilla ◽  
I. Armas-Rivera ◽  
O. Pottiez ◽  
M.V. Andrés ◽  
...  

2019 ◽  
Vol 58 (2) ◽  
pp. 020910 ◽  
Author(s):  
Xing Luo ◽  
Tong Hoang Tuan ◽  
Than Singh Saini ◽  
Hoa Phuoc Trung Nguyen ◽  
Takenobu Suzuki ◽  
...  

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