Theoretical Analysis of a Acoupled Fiber Ring Resonator

2013 ◽  
Vol 397-400 ◽  
pp. 765-771
Author(s):  
Xiao Min Zhang ◽  
Yan Ke Ci ◽  
Jin Li Yao ◽  
Jing Li Wang

A fiber ring is very commonly used to generate stimulated Brillouin scatterings(SBS), especially by using fiber ring resonator. In this paper we theoretically analyzed some parameters of our interest in a coupled fiber ring resonator. We firstly analyzed a directional coupler, determined the optical power distribution among the four ports of the coupler. Then theoretically analyzed the transmission function of a coupled fiber ring resonator, followed by the simulation of the analysis. The simulation results show that the smaller the coupling coefficient is, the better the cavity finesse and extinction ration are, the lower the SBS threshold is, which is of great importance when it comes to the generation of SBS.

2014 ◽  
Vol 496-500 ◽  
pp. 918-921
Author(s):  
Xiao Min Zhang ◽  
Yan Ke Ci ◽  
Jin Li Yao

Fiber ring resonator is widely used to generate stimulated Brillouin scattering(SBS). In this paper, the operation principle of SBS in a single mode fiber ring is analyzed, and the simulation method is proposed.


1984 ◽  
Author(s):  
Ming H. Yu ◽  
David B. Hall

1999 ◽  
Vol 256 (1) ◽  
pp. 47-54 ◽  
Author(s):  
Henning U. Voss ◽  
Andreas Schwache ◽  
Jürgen Kurths ◽  
Fedor Mitschke

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.


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